international atomic energy agency nuclear data services

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INTERNATIONAL ATOMIC ENERGY AGENCY NUCLEAR DATA SERVICES DOCUMENTATION SERIES OF THE IAEA NUCLEAR DATA SECTION IAEA-NDS-206 Rev. 2000/09 BNL-NCS-63380- 2000/05 Rev. EXFOR Basics A Short Guide to the Nuclear Reaction Data Exchange Format Victoria McLane National Nuclear Data Center Brookhaven National Laboratory Upton, NY 11973-5000, USA Abstract: EXFOR is the agreed exchange format for the transmission of experimental nuclear reaction data between national and international nuclear data centers for the benefit of nuclear data users in all countries. This report is intended as a guide to data users. For a complete guide to the EXFOR system see: EXFOR Systems Manual, IAEA-NDS-207 (BNL- NCS-63330-00/04-Rev.) Nuclear Data Section e-mail, INTERNET: [email protected] International Atomic Energy Agency fax: (43-1)26007 P.O. Box 100 cable: INATOM VIENNA a A-1400 Vienna telex: 1-12645 atom a Austria telephone: (43-1)2600-21710 online: TELNET or FTP: IAEAND.IAEA.ORG usernames: IAEANDS for interactive Nuclear Data Information System ANONYMOUS for FTP file transfer FENDL2 for FTP file transfer of FENDL-2.0 files RIPL for FTP file transfer of RIPL NDSONL for FTP access to files sent to NDIS “open” area For users with web-browsers: http://www-nds.iaea.org

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INTERNATIONAL ATOMIC ENERGY AGENCY

NUCLEAR DATA SERVICESDOCUMENTATION SERIES OF THE IAEA NUCLEAR DATA SECTION

IAEA-NDS-206Rev. 2000/09BNL-NCS-63380-

2000/05 Rev.

EXFOR Basics

A Short Guide to theNuclear Reaction Data Exchange Format

Victoria McLaneNational Nuclear Data Center

Brookhaven National LaboratoryUpton, NY 11973-5000, USA

Abstract: EXFOR is the agreed exchange format for the transmission of experimentalnuclear reaction data between national and international nuclear data centers for the benefit ofnuclear data users in all countries. This report is intended as a guide to data users. For acomplete guide to the EXFOR system see: EXFOR Systems Manual, IAEA-NDS-207 (BNL-NCS-63330-00/04-Rev.)

Nuclear Data Section e-mail, INTERNET: [email protected] Atomic Energy Agency fax: (43-1)26007P.O. Box 100 cable: INATOM VIENNA aA-1400 Vienna telex: 1-12645 atom aAustria telephone: (43-1)2600-21710

online: TELNET or FTP: IAEAND.IAEA.ORGusernames: IAEANDS for interactive Nuclear Data Information System

ANONYMOUS for FTP file transferFENDL2 for FTP file transfer of FENDL-2.0 filesRIPL for FTP file transfer of RIPLNDSONL for FTP access to files sent to NDIS “open” area

For users with web-browsers: http://www-nds.iaea.org

Note:

The IAEA-NDS-reports should not be considered as formal publications. When a nuclear datalibrary is sent out by the IAEA Nuclear Data Section, it will be accompanied by an IAEA-NDS-report which should give the data user all necessary documentation on contents, format andorigin of the data library.

IAEA-NDS-reports are updated whenever there is additional information of relevance to theusers of the data library.

For citations care should be taken that credit is given to the author of the data library and/or tothe data center which issued the data library. The editor of the IAEA-NDS-report is usually notthe author of the data library.

Neither the originator of the data libraries nor the IAEA assume any liability for their correctnessor for any damages resulting from their use.

96/11

Citation guideline:

When quoting EXFOR data in a publication this should be done in the following way:

"A.B. Author et al.: Data file EXFOR-12345.002 dated 1980-04-05, compare J. Nucl. Phys. 12,345, (1979). EXFOR data received from the IAEA Nuclear Data Section, Vienna."

EXFOR Basics

A Short Guide to the

Nuclear Reaction Data Exchange Format

Victoria McLane

National Nuclear Data Center

on behalf of the

Nuclear Data Center Network

May 2000

Brookhaven National Laboratory

Upton, NY 11973-5000

BNL-NCS-63380-2000/05-Rev.IAEA-NDS-206INFORMAL REPORT

DISCLAIMER

This report was prepared as an account of work sponsored by an agency of the United StatesGovernment. Neither the United States Government nor any agency thereof, nor any of their employees, norany of their contractors, subcontractors, or their employees, makes any warranty, express or implied, orassumes any legal liability or responsibility for the accuracy, completeness, or usefulness of any information,apparatus, product, or process disclosed, or represents that its use would not infringe privately owned rights.Reference herein to any specific commercial product, process, or service by trade name, trademark,manufacturer, or otherwise, does not necessarily constitute or imply its endorsement, recommendation, orfavoring by the United States Government or any agency, contractor, or subcontractor thereof. The viewsand opinions of authors expressed herein do not necessarily state or reflect those of the United StatesGovernment or any agency, contractor, or subcontractor thereof.

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Table of Contents

Page

INTRODUCTION........................................................................................................................... 1

EXCHANGE FILE FORMAT........................................................................................................ 2Permitted character set ........................................................................................................ 3EXFOR Records.................................................................................................................. 3System identifiers................................................................................................................ 4

POINTERS...................................................................................................................................... 5

BIB SECTION ................................................................................................................................ 6Information-identifier keywords ......................................................................................... 6Coded (machine-retrievable) information........................................................................... 6Free text............................................................................................................................... 7Coding of nuclides and compounds .................................................................................... 7

COMMON AND DATA SECTIONS (Data Tables)...................................................................... 8COMMON section .............................................................................................................. 9DATA section ..................................................................................................................... 9

APPENDIX A. Nuclear Reaction Data Centers

APPENDIX B. Information-Identifier Keywords

APPENDIX C. List of Dictionaries

APPENDIX D. Covariance Data File Format

APPENDIX E. Example of an EXFOR Entry

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Acknowledgements

This work was performed under the auspices of the U. S. Department of Energy, Division ofNuclear Physics, Office of Science.

The author would like to thank the members of the Nuclear Data Center Network, especially, H.D. Lemmel and O. Schwerer of the International Atomic Energy Agency Nuclear Data Section,and S. Maev of the Russian Nuclear Data Center for their contributions.

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INTRODUCTION

This manual is intended as a guide to users of nuclear reaction data compiled in the EXFOR format,and is not intended as a complete guide to the EXFOR System.1

EXFOR is the exchange format designed to allow transmission of nuclear reaction data between theNuclear Reaction Data Centers.2 In addition to storing the data and its’ bibliographic information,experimental information is also compiled. The status (e.g., the source of the data) and history (e.g.,date of last update) of the data set is also included.

EXFOR is designed for flexibility in order to meet the diverse needs of the nuclear reaction datacenters. It was originally conceived for the exchange of neutron data and was developed throughdiscussions among personnel from centers situated in Saclay, Vienna, Livermore and Brookhaven. Itwas accepted as the official exchange format of the neutron data centers at Saclay, Vienna, Brookhavenand Obninsk, at a meeting held in November 1969.3 As a result of two meetings held in 1975 and19764 and attended by several charged-particle data centers, the format was further developed andadapted to cover all nuclear reaction data.

The exchange format should not be confused with a center-to-user format. Although users may obtaindata from the centers in the EXFOR format, other center-to-user formats have been developed to meetthe needs of the users within each center’s own sphere of responsibility.

The EXFOR format, as outlined, allows a large variety of numerical data tables with explanatory andbibliographic information to be transmitted in a format:• that is machine-readable (for checking and indicating possible errors);• that can be read by personnel (for passing judgement on and correcting errors).

The data presently included in the EXFOR exchange file include:• a "complete" compilation of experimental neutron-induced reaction data,• a selected compilation of charged-particle-induced reaction data,• a selected compilation of photon-induced reaction data.

1 For a complete guide to the EXFOR System, see EXFOR Systems Manual, Brookhaven National Laboratory

report BNL-NCS-63330 (1999).2 See Appendix A for a list of the Nuclear Reaction Data Centers and their areas of responsibilities.3 See IAEA report INDC(NDS)-16/N (December 1969).4 See IAEA report INDC(NDS)-69 (December 1975) and INDC(NDS)-77 (October 1976).

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EXCHANGE FILE FORMAT

An exchange file contains a number of entries (works). Each entry is divided into a number ofsubentries (data sets). Each entry is assigned an accession number; each subentry is assigned asubaccession number (the accession number plus a subentry number). The subaccession numbers areassociated with a data table throughout the life of the EXFOR system.

The subentries are further divided into:• bibliographic, descriptive and bookkeeping information (hereafter called BIB information),• common data that applies to all data throughout the subentry , and• a data table.

The file may, therefore, be considered to be of the following form:

File Entry Subentry

Bibliographic

Information

Common

Data

Data

Table

In order to avoid repetition of information that is common to all subentries within an entry or to alllines within a subentry, information may be associated with an entire entry or with an entire subentry.To accomplish this, the first subentry of each work contains only information that applies to all othersubentries. Within each subentry, the information common to all lines of the table precedes thetable. Two levels of hierarchy are thereby established:

Entry SubentriesBibliographicInformationCommon

Subentry Common Data

BibliographicInformationCommon Data

DataSubentry

Data Table

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Permitted Character Set. The following characters are permitted for use in the exchange format:

All Roman characters, A to Z and a to zAll numbers, 0 to 9The special characters:

+ (plus)- (minus). (decimal point/full stop)) (right parenthesis)( (left parenthesis)* (asterisk)/ (slash)= (equals)’ (apostrophe), (comma)% (percent)< (less than)

> (greater than): (colon); (semi-colon)! (exclamation mark)? (question mark)& (ampersand)

# (number symbol)[ (opening bracket)] (closing bracket)" (quotation mark)~ (varies as sign)@ (at symbol)

EXFOR Records

EXFOR Exchange files consist of 80 character ASCII records. The format of columns 1-66 variesaccording to the record type as outlined in the following chapters. Columns 67-79 is used to uniquelyidentify a record within the file. The records on the file are in ascending order according to the recordidentification. Column 80 is reserved for an alteration flag.

Record identification. The record identification is divided into three fields: the accession number(entry), subaccession number (subentry), and record number within the subentry. The format of thesefields is as follows.

Columns 67-71 Center-assigned accession number

72-74 Subaccession number

75-79 Sequence number

Alteration flag (column 80). The last column of each record contains the alteration flag which is usedto indicate that a record and/or following records has been altered (i.e., added, deleted or modified)since the work was last transmitted. The flag field will normally contain a blank to indicate anunaltered record.

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System Identifiers

Each of the sections of an EXFOR file begins and ends with a system identifier. Each of thefollowing system identifiers indicates the beginning of one of these sections.

TRANS - A file is the unitENTRY - An entry is the unitSUBENT - A subentry is the unitBIB - A BIB Information section is the unitCOMMON - A common data section is the unitDATA - A data table section is the unit

• The end of unit is signaled by modifier END preceding the basic system identifier, e.g.,NODATA.

• A positive indication that a unit is intentionally omitted is signaled by the modifier NO

preceding the basic system identifier, e.g., NOSUBENT.

The following system identifiers are defined.

1. A file is:Headed by: TRANS cxxx yyyymmdd

CXXX = the center-identification character,5

yyyymmdd = date (year, month, and day) on which the file was generated.Ended by: ENDTRANS N1

N1 = number of entries (accession numbers) on the file.

2. An entry is:Headed by: ENTRY N1 N2

N1 = 5-character accession numberN2 = Date of last update (or date of entry if never updated) (yyyymmdd)

Ended by: ENDENTRY N1N1 - The number of subentries in the work.6

N2 - Presently unused (may be blank or zero).

3. A subentry is:Headed by: SUBENT N1 N2

N1 = 8-character subaccession number (accession number and subentry number).N2 = Date of last update (or date of entry if never updated) (yyyymmdd).

Ended by: ENDSUBENT N1N1 - The number of records within the subentry.

If a subentry has been deleted, the following record is included in the fileNOSUBENT N1 N2

N1 = 8-character subaccession number.N2 = Date of last alter.

5 On files that contain entries with different file-identification characters, column 67 is assignedsuch that the record sorts at the beginning of the file.6 NOSUBENT records are counted as subentries when computing the number of subentries in anentry.

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4. A BIB section is:Headed by BIB N1 N2

N1 =Number of information-identifier keywords in the BIB section.N2 = Number of records in the BIB section.

Ended by : ENDBIB N1N1 - Number of records in BIB section.

If no BIB section is given the following record is included:NOBIB

5. A COMMON section is:Headed by: COMMON N1 N2

N1 = Number of common data fields.N2 = Number of records within the common section.

Ended by: ENDCOMMON N1

N1 = Number of records within the common section.If no COMMON section is given, the following record is included:

NOCOMMON

6. A DATA section is:Headed by: DATA N1 N2

N1 = Number of fields (variables) associated with each line of a data table.N2 = Number of data lines within the table (excluding headings and units).

Ended by: ENDDATA N1

N1 - Number of records within the data section.If no DATA section is given, the following record is included:

NODATA

POINTERS

Different pieces of EXFOR information may be linked together by pointers. A pointer is a numericor alphabetic character (1,2...9,A,B,...Z) placed in the eleventh column of the information-identifierkeyword field in the BIB section and in the field headings in the COMMON or DATA section.

Pointers may link, for example,• one of several reactions with its data field;• one of several reactions with a specific piece of information in the BIB section (e.g., ANALYSIS),

and/or with a value in the COMMON section, and/or with a field in the DATA section;• a value in the COMMON section with any field in the DATA section.

In general, a pointer is valid for only one subentry. A pointer used in the first subentry applies to allsubentries and has a unique meaning throughout the entire entry.

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BIB SECTION

The BIB section contains the bibliographic information (e.g., reference, authors), descriptiveinformation (e.g., neutron source, method, facility), and administrative information (e.g., history)associated with the data presented. It is identified on an exchange file as that information betweenthe system identifiers BIB and ENDBIB.

A BIB record consists of three parts:

columns 1-11: information-identifier keyword field,columns 12-66: information field, which may contain coded information and/or free text,columns 67-80: record identification and alteration flag fields.

BIB information for a given data set consists of the information contained in the BIB section of itssubentry together with the BIB information in subentry 001. That is, information coded in subentry001 applies to all other subentries in the same entry. A specific information-identifier keyword maybe included in either subentry or both.

Information-identifier keywords

The information-identifier keyword is used to define the significance of the information given incolumns 12-66. The keyword is left adjusted to begin in column 1, and does not exceed a length of10 characters (column 11 is either blank, or contains a pointer, see Chapter 5).

These keywords may, in general, appear in any order within the BIB section, however, aninformation-identifier keyword is not repeated within any one BIB section. If pointers are present,they appear on the first record of the information to which they are attached and are not repeated oncontinuation records. A pointer is assumed to refer to all BIB information until either anotherpointer or a new keyword is encountered. As this implies, pointer-independent information for eachkeyword appears first.

Coded (machine-retrievable) information

Coded information may be used:• to define the actual BIB information,• as a link to the COMMON and DATA section,• to enter associated numerical data.

Coded information is enclosed in parentheses and left adjusted so that the opening parenthesisappears in column 12. Several pieces of coded information may be associated with a giveninformation-identifier keyword.

Codes for use with a specific keyword are found in the relevant dictionary. However, for somekeywords, the code string may include retrievable information other than a code from one of thedictionaries.

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7

In general, codes given in the dictionaries may be used singly or in conjunction with one or morecodes from the same dictionary. Two options exist if more than one code is used:

a) two or more codes within the same set of parenthesis, separated by a comma;Example: (SOLST,NAICR)

b) each code on a separate record, enclosed in it’s own set of parenthesis starting in column 12,followed by free text.

Example: (SOLST) free text(NAICR) free text

For some cases, the information may be continued onto successive records. Information oncontinuation records does not begin before column 12 (columns 1-10 are blank and column 11 isblank or contains a pointer).

Note that some information-identifier keywords have no coded information associated with them andthat, for many keywords which may have coded information associated with them, it need not alwaysbe present.

Free text

Free text may be entered in columns 12-66 under each of the information-identifier keywords in theBIB section. The text follows any coded information on the record or may begin on a separaterecord; it may be continued onto any number of records.

The language of the free text is English.

Coding of nuclides and compounds.

Nuclides appear in the coding of many keywords. The general code format is Z-S-A-X, where:Z is the charge number; up to 3 digits, no leading zerosS is the element symbol; 1 or 2 characters (Dictionary 8)A is the mass number; up to 3 digits, no leading zeroes. A single zero denotes natural isotopic

composition.X is an isomer code denoting the isomeric state; this subfield is not used if there are no known

isomeric states.X may have the following values:G for ground state (of a nucleus which has a metastable state)M if only one metastable state is regardedM1 for the first metastable stateM2 for the second, etc.T for sum of all isomers (limited to use within an isomeric ratio in SF4 of the reaction

string)

Examples: 92-U-23549-IN-115-M/T

Compounds may in some cases replace the nuclide code. The general format for coding compoundsis either the specific compound code, taken from Dictionary 9, or the general code for a compoundof the form Z-S-CMP.

Example: 26-FE-CMP

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COMMON AND DATA SECTIONS

A data table is, generally, a function of one or more independent variables, e.g.,

• X vs. Y, e.g., energy, cross section• X, X′ and Y, e.g., energy and angle; differential cross section• X, X′ and X″ vs. Y, e.g., energy, secondary energy, angle, partial angular distribution.

When more than one representation of Y is present, the table may be X vs. Y and Y′, with associatederrors for X, Y and Y′ (e.g., X = energy, Y = absolute cross section, Y′ = relative cross section), andpossible associated information. The criteria for grouping Y with Y′ are that they both be derived fromthe same experimental information by the author of the data.

For some data, the data table does not have an independent variable X but only a function Y. (Examples: Spontaneousν; resonance energies without resonance parameters)

Additional variables may be associated with the data, e.g., errors, standards.

The format of the common data (COMMON) and data table (DATA) sections is identical. Eachsection is a table of data containing the data headings and units associated with each field. Thedifference between the common data and data table is:

• The common data contains constant parameters that apply to each line of a point data table;

• The data table contains fields of information; each field, generally, contains values as a functionof one or more independent variables (e.g., angle, angular error, cross section, cross sectionerror), i.e., one or more lines of data.

Each physical record may contain up to six information fields, each 11 columns wide. If more thansix fields are used, the remaining information is contained on the following records. Therefore, adata line consists of up to three physical records. The number of fields in a data line is restricted to18.

Records are not packed; rather, individual point information is kept on individual records; i.e., if onlyfour fields are associated with a data line, the remaining two fields are left blank, and, in the case ofthe data table, the information for the next line begins on the following record. These rules also applyto the headings and units associated with each field.

The content of the COMMON and DATA sections are as follows:

• Field headings: a data heading left adjusted to the beginning of each field (columns 1, 12, 23, 34,45, 56), plus, perhaps, a pointer placed in the last (11th) column of a field.

• Data units: left adjusted to the beginning of each field (columns 1, 12, 23, 34, 45, 56).

• Numerical data: FORTRAN-readable using a floating-point format, as follows.• A decimal point is always present, even for integers.• A decimal number without an exponent can have any position within the 11-character field.• No blank is allowed following a sign (+ or -).• A plus sign may be omitted, except that of an exponent when there is no E.

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• In an exponential notation, the exponent is right adjusted within the 11-character field. Themantissa may have any position.

The values are either zero or have absolute values between 1.0000E-38 and 9.999E+38.

COMMON Section

The COMMON section is identified as that information between the system identifiers COMMON andENDCOMMON. In the common data table, only one value is entered for a given field, and successivefields are not integrally associated with one another.

An example of a common data table with more than 6 fields:

1 12 23 34 45 56 66COMMONEN EN-ERR EN-RSL E-LVL E-LVL MONITMONIT-ERRMEV MEV MEV MEV MEV MBMB2.73 0.02 0.05 2.73 2.78 3.4560.123ENDCOMMON

DATA Section

The DATA section is identified as that information between the system identifiers DATA andENDDATA. In the DATA table, all entries on a record are integrally associated with an individualpoint. Independent variables precede dependent variables, and are monotonic until the value of thepreceding independent variable, if any exist, changes.

Every line in a data table gives data information. This means, for example, that a blank in a fieldheaded DATA is permitted only when another field contains the data information on the same line,e.g., under DATA-MAX. In the same way, each independent variable occurs at least once in each line(e.g., either under data headings E-LVL or E-LVL-MIN, E-LVL-MAX, see example following). Supplementary information, such as resolution or standard values, is not given on a line of a datatable unless the line includes data information. Blanks are permitted in all fields.

An example of a point data table is shown below with its associated DATA and ENDDATA records.

1 12 23 34 45 56 66DATAANG ANG-ERR DATA DATA-ERR DATA-MAXADEG ADEG MB/SR MB/SR MB/SR10.7 1.8 138. 8.522.9 1.2 127. 4.239.1 0.9 83.246.7 0.7 14.8 2.9ENDDATA

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EXFOR Basics

A.1

Appendix A

Nuclear Reaction Data Centers

This appendix contains a list of the members of the Nuclear Data Center Network, along withinformation on how to contact them. Also list are the entry series for which each of the datacenters is responsible.

EXFOR Basics

A.2

EXFOR Basics

A.3

Principal Centers and their services areas.1

United States and Canada

National Nuclear Data Center,Bldg. 197DBrookhaven National LaboratoryUpton, NY, 11973-5000 U.S.A.

Center codes: 1, C, L, P, TTelephone: +1 631-344-2902Fax: +1 631-344-2806Email: [email protected]

or [email protected]

www.nndc.bnl.gov

O. E. C. D. Nuclear Energy Agency Member Countries

NEA Data Bank12, boulevard des Iles92130 Issy-les-Moulineaux,FRANCE

Center codes: 2, OTelephone: +33 (1) 4524 1071Fax: +33 (1) 4524 1110Email:[email protected]

or [email protected]

Countries of the former Soviet Union

Federal Research Center IPPECentr Yadernykh DannykhPloschad Bondarenko249 020 Obninsk, Kaluga Region,RUSSIA

Center codes: 4, QTelephone: +7 084-399-8982Fax: +7 095-883-3112Email: [email protected]

Remaining countries

IAEA Nuclear Data SectionWagramerstr. 5, P.O.Box 100A-1400 Vienna, AUSTRIA

Center codes: 3, D, G, V.Telephone: +43 (1) 2360 1709Fax: +43 (1) 234 564Email: [email protected]

Other participating centers.

National Scientific Research CenterKurchatov InstituteRussia Nuclear Center46 Ulitsa Kurchatova123 182 Moscow, RUSSIA

Center codes: A, BEmail: [email protected]

Institute of Nuclear PhysicsMoskovskiy Gos. UniversitetVorob’evy Gory119 899 Moscow, RUSSIA

Center code: MEmail: [email protected]

1 The four principal centers are responsible for maintaining customer services for the area given.2 nn = first and last initial of person to be contacted, e.g., [email protected].

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A.4

China Nuclear Data CenterChina Institute of Atomic EnergyP.O. BOX 275 (41)Beijing 102413, CHINA

Center code: SEmail: [email protected]

Japan Charged Particle Reaction GroupDept. of PhysicsHokkaido UniversityKita-10 Nisha-8, Kita-kuSapporo 060, JAPAN

Center code: E, REmail: [email protected]

Dr. F. T. TárkányiCyclotron Application DepartmentATOMKI, Institute of Nuclear ResearchBem Tér 18/c, P. O. Box 51H-4001 Debrecen, HUNGARY

Contributes data under center code DEmail: [email protected]

Russian Federal Center - VNIIEFSarov, Nizhni Novgorod Region607 190 pr. Mira 37, RUSSIA

Center code: FEmail: [email protected]

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B.1

Appendix B

Information Identifier Keywords

This appendix provides a listing of all information-identifier keywords, along with details abouttheir use. The keywords appear in alphabetical order.

EXFOR Basics

B.2

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B.3

ADD-RES. Gives information about any additional results obtained in the experiment, butwhich are not compiled in the data tables. Codes are given in Dictionary 20.Example: ADD-RES (RANGE) Range of recoils measured.

ANALYSIS. Gives information as to how the experimental results have been analyzed to obtainthe values given under the heading DATA which actually represent the results of the analysis.Codes are found in Dictionary 23.

Example: ANLAYSIS (MLA) Breit-Wigner multilevel analysis

ASSUMED Gives information about values assumed in the analysis of the data, and aboutCOMMON or DATA fields headed by ASSUM or its derivatives. The format of the code is:

(heading,reaction,quantity)

Heading field: data heading to be defined.

Reaction field and quantity field: coded as under the keyword REACTION.

Example:ASSUMED (ASSUM,6-C-12(N,TOT),,SIG)

AUTHOR. Gives the authors of the work reported.

Example:

AUTHOR (R.W.McNally Jr,A.B.JONES)

COMMENT. Gives pertinent information which cannot logically be entered under any other ofthe keywords available.

CORRECTION. Gives information about corrections applied to the data in order to obtain thevalues given under DATA. See also LEXFOR, Correction.

COVARIANCE. Gives covariance information provided by the experimentalist, or to flag theexistence of a covariance data file. See Appendix C for covariance file format.Example: COVARIANCE (COVAR) COVARIANCE FILE EXISTS AND MAY BE OBTAINED ON

REQUEST.

CRITIQUE. Gives comments on the quality of the data presented in the data table.

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B.4

DECAY-DATA. Gives the decay data for any nuclide occurring in the reaction measured asassumed or measured by the author for obtaining the data given1. The general format of thecoding string consists of three major fields which may be preceded by a decay flag:

((decay flag)nuclide,half-life,radiation).

Flag. A fixed-point number that also appears in the data section under the data headingDECAY-FLAG. If the flag may be omitted, its parentheses are also omitted.

Nuclide field. A nuclide code.

Half-life field. The half-life of the nuclide specified, coded as a floating-point number,followed by a unit code with the dimensions of TIME.

Radiation field. Consists of three subfields: (type of radiation, energy, abundance) This fieldmay be omitted, or repeated (each radiation field being separated by a comma). The absenceof any subfield is indicated by a comma; trailing commas are not included.

SF1. Type-of-radiation. A code from Dictionary 13. Where two or more different decaymodes are possible and are not distinguished in the measurement, two or more codes aregiven; each separated by a slash. (See Example b, following).

SF2. Energy. The energy of the radiation in keV, coded as a floating-point number. Inthe case of two or more unresolved decays, two or more energies, or a lower and upperenergy limit, are given, each separated by a slash. (See Example e).

SF3. Abundance. The abundance of the observed per decay, coded as a floating-pointnumber.

Examples

a) DECAY-DATA (60-ND-140,3.3D) (radiation field omitted)

b) DECAY-DATA (59-PR-140,,B+/EC,,0.500) (half-life and decay energy omitted)

c) DECAY-DATA (25-MN-50-G,0.286SEC,B+,6610.) (abundance omitted)

d) DECAY-DATA ((1.)60-ND-138,5.04HR,DG,328.,0.065) (decay flag, all fieldspresent)

e) DECAY-DATA (60-ND-139-M,5.5HR,DG,708./738.,0.64) (the abundance given isthe total abundance of both γ rays)

f) DECAY-DATA (60-ND-139-G,30.0MIN,B+,,0.257,DG,405.,0.055)

(60-ND-139-M,5.5HR, DG,738.,0.37,DG,982.,0.29,DG,708.,0.27,DG,403.,0.03,B+,,0.006)

1 Decay data relevant to the monitor reaction are coded under the keyword DECAY-MON and not under DECAY-DATA.

EXFOR Basics

B.5

DECAY-MON. Gives the decay data assumed by the author for any nuclide occurring in themonitor reaction used. The coding rules are the same as those for DECAY-DATA, except thatthere is no flag field.

DETECTOR. Gives information about the detector(s) used in the experiment. Codes are foundin Dictionary 22. If the code COIN is used, then the codes for the detectors used in coincidencefollow within the same parenthesis;

Example: DETECTOR (COIN,NAICR,NAICR)

EMS-SEC. Gives information about secondary squared effective mass of a particle or particlesystem, and to define secondary-mass fields given in the data table. The format of the codedinformation is: (heading, particle).

Heading Field contains the data heading or the root2 of the data heading to be defined.Particle Field contains the particle or nuclide to which the data heading refers. The code is:

either a particle code from Dictionary 13.or a nuclide code.

Example: EMS-SEC (EMS1,N)(EMS2,P+D)

EN-SEC. Gives information about secondary energies, and to define secondary-energy fieldsgiven in the data table. The format of the coded information is: (heading,particle).

Heading Field. Contains the data heading or the root of the data heading to be defined.

Particle Field. Contains the particle or nuclide to which the data heading refers. The code is:either a particle code from Dictionary 13.or a nuclide code.

Example: EN-SEC (E1,G)(E2,N)(E-EXC,3-LI-7

ERR-ANALYS. Explains the sources of uncertainties and the values given in the COMMON orDATA sections under data headings of the type ERR- or -ERR. The general code format is(heading,correlation factor) free text

Heading Field. Contains the data heading or the root3 of the data heading to be defined.

Correlation Factor Field contains the correlation factor, coded as a floating point number.

Example:

BIB…ERR-ANALYS (EN-ERR) followed by explanation of energy error

(ERR-T) followed by explanation of total uncertainty(ERR-S) followed by explanation of statistical uncertainty

2 Root means that the data heading given will also define the same heading followed by -MIN, -MAX or -APRX.3 Root means that the data heading given also defines the heading preceded by + or -.

EXFOR Basics

B.6

EXP-YEAR. Defines the year in which the experiment was performed when it differssignificantly from the data of the references given (e.g., classified data published years later).

Example: EXP-YEAR (1965)

FACILITY. Defines the main apparatus used in the experiment. The facility code fromDictionary 18 may be followed by an institute code from Dictionary 3, which specifies thelocation of the facility.

Example: FACILITY (CHOPF,1USACOL)(SPECC,1USABNL)

FLAG. Provides information to specific lines in a data table. See also LEXFOR, Flags.

Example: BIB

FLAG (1.) Data averaged from 2 runs

(2.) Modified detector used at this energy

ENDBIB

DATA

EN DATA FLAG

KEV MB NO-DIM

1.2 123. 1.

2.3 234.

3.4 456. 2.

ENDDATA

HALF-LIFE. Gives information about half-life values and defines half-life fields given in thedata table. The general coding format is: (heading,nuclide)

Example: HALF-LIFE (HL1,41-NB-94-G)(HL2,41-NB-94-M)

HISTORY. Documents the handling of an entry or subentry. The general format of the code is:(yyyymmddX), where yyyymmdd is the date (year,month,day) and X is a code from Dictionary15.

Example: HISTORY (19940312C)(19960711A) Data units correcte d.

INC-SOURCE. Gives information on the source of the incident particle beam used in theexperiment. Codes are found in Dictionary 19.

Example: INC-SOURCE (POLNS,D-T)INC-SOURCE (MPH=13-AL-27(N,A)11-NA-24)

INC-SPECT. Provides free text information on the characteristics and resolution of theincident-projectile beam.

EXFOR Basics

B.7

INSTITUTE. Designates the laboratory, institute, or university at which the experiment wasperformed, or with which the authors are affiliated. Codes are given in Dictionary 3.

Examples: INSTITUTE (1USAGA, 1USALAS)INSTITUTE (2FR SAC)

LEVEL-PROP. Gives information on the spin and parity of excited states. The general formatof the code is ((flag) nuclide, level identification, lever properties)

Flag. Coded as a fixed-point number that appears in the data section under the data headingLVL-FLAG. When the flag is omitted, its parentheses are also omitted.

Nuclide. Coded is a nuclide, except that the use of the extension G is optional.

Level identification. Identification of the level whose properties are specified, given as eithera level energy or level number. If the field omitted, its separating comma is omitted.

Level Energy. The field identifier E-LVL= followed by the excited state energy in MeV,coded as a floating-point number which also appears in the data section under the dataheading E-LVL.

Level Number. The field identifier LVL-NUMB= followed by the level number of theexcited state, coded as a fixed-point number which also appears in the data section underthe data heading LVL-NUMB.

Level properties. Properties for the excited state, each preceded by a subfield identification.At least one of the fields must be present. If the field is omitted, its separating comma isomitted.

Spin. The field identifier SPIN=, followed by the level spin coded as a floating pointnumber. For an uncertain spin assignment, two or more spins may be given, eachseparated by a slash.

Parity. The field identifier PARITY=, followed by the level parity, coded as e.g., +1. or -1.

Examples:LEVEL-PROP (82-PB-206,E-LVL=0.,SPIN=0./1.,PARITY=+1.)

(82-PB-206,E-LVL-1.34,SPIN+3.,PARITY=+1.)LEVEL-PROP ((1.)82-PB-206,,SPIN=0./1.,PARITY=+1.)

((2.)82-PB-206,,SPIN=3.,PARITY=+1.)LEVEL-PROP (82-PB-207,LVL-NUMB=2.,SPIN=1.5,PARITY=-1)

METHOD. Describes the experimental technique(s) employed in the experiment. Codes arefound in Dictionary 21.

Example: METHOD (RCHEM) Radiochemical separation

MISC-COL. Defines fields in the COMMON or DATA sections headed by MISC and itderivatives.

Example: MISC-COL (MISC1) Free text describing 1st miscellaneous field(MISC2) Free text describing 2nd miscellaneous field

EXFOR Basics

B.8

MOM-SEC. Gives information about secondary linear momentum, and defines secondary-momentum fields given in the data table. The general code format is: (heading,particle)

Heading Field: the data heading or root4 of the data heading to be defined.

Particle Field: the particle or nuclide to which the data heading refers. The code is:either a particle code from Dictionary 13.or a nuclide code.

Example: MOM-SEC (MOM-SEC1,26-FE-56)(MOM-SEC2,26-FE-57)

MONITOR. Gives information about the standard reference data (standard, monitor) used inthe experiment and defines information coded in the COMMON and DATA sections under thedata heading MONIT, etc. The general coding format is ((heading) reaction)

Heading Field. Contains the data heading of the field in which the monitor value is given. Ifthe heading is omitted, its parenthesis is omitted.

Reaction Field. The coding rules are identical to those for REACTION, except that subfields 5to 9 may be omitted if the reaction is known.

Example:REACTION 1 (AAAAA)

2 (BBBBB)MONITOR 1 (CCCCC)

2 (DDDDD)…DATAEN DATA 1 DATA 2 MONIT 1 MONIT 2…

MONIT-REF. Gives information about the source reference for the standard (or monitor) dataused in the experiment.

The general code format is ((heading)subaccession#,author,reference)

Heading Field: Data heading of the field in which the standard value is given. If the headingis omitted, its parentheses are also omitted.

Subaccession Number Field: Subaccession number for the monitor data, if the data is givenin an EXFOR entry. Cnnnn001 refers to the entire entry; Cnnnn000 refers to a yet unknownsubentry.

Author Field. The first author, followed by "+" when more than one author exists.

Reference Field. May contain up to 6 subfields, coded as under REFERENCE.

Example:MONIT-REF ((MONIT1)BOO17005,J.GOSHAL,J,PR,80,939,1950)

((MONIT2),A.G.PANONTIN+,J,JIN,30,2017,1968)

4 Root means that the data heading given will also define the same heading followed by -MIN, -MAX or -APRX.

EXFOR Basics

B.9

PART-DET. Gives information about the particles detected directly in the experiment.Particles detected in a standard/monitor reaction are not coded under this keyword. The code iseither a code from Dictionary 13, or, for particles heavier than α particles, a nuclide code.Particles detected pertaining to different reaction units within a reaction combination are codedon separate records in the same order as the corresponding reaction units.

Example: PART-DET (A)PART-DET (3-LI-6)

RAD-DET. Gives information about the decay radiations (or particles) and nuclides observed inthe reaction measured. The general format of the code is ((flag)nuclide, radiation).

Flag is a fixed-point number which appears in the data section under the data headingDECAY-FLAG. If the field is omitted, its parentheses are also omitted.

Nuclide contains a nuclide code.

Radiation contains one or more codes from Dictionary 33, each separated by a comma.

Examples:RAD-DET (25-MN-52-M,DG,B+)RAD-DET (48-CD-115-G,B-)

(49-IN-115-M,DG)RAD-DET ((1.)48-CD-115-G,B-)

((2.)49-IN-115-M,DG)

REACTION. Specifies the data presented in the DATA section in fields headed by DATA.5 Thegeneral format of the code is (reaction, quantity, data-type).

Reaction field. The reaction field consists of 4 subfields.

SF1. Target nucleus. Contains either:a) a nuclide code.

A = 0 denotes natural isotopic abundance.b) a compound code.c) a variable nucleus code ELEM and/or MASS

Example: (ELEM/MASS(0,B-),,PN)

SF2. Incident projectile. Contains one of the following:

a) a particle code from Dictionary 28.b) for particles heavier than an α, a nuclide code.

SF3. Process. Contains one of the following:

a) a process code from Dictionary 30, e.g., TOT.b) a article code from Dictionary 29 which may be preceded by a multiplicity factor, whose

value may be 2→99.6, e.g., 4A.

5 And similar headings such as DATA-MIN, DATA-MAX, etc.6 In the few cases where the multiplicity factor may exceed 99, the Variable Number of Emitted NucleonsFormalism may be used, see page 6.7.

EXFOR Basics

B.10

c) for particles heavier than α, a nuclide code.Examples: 8-O-16

8-O-16+8-O-16

d) combinations of a), b) and c), with the codes connected by ‘+’.Examples: HE3+8-0-16

A+XN+YP

If SF5 contains the branch code UND7 (undefined), the particle codes given in SF3 represent only

the sum of emitted nucleons, implying that the product nucleus coded in SF4 has been formedvia different reaction channels. The code (DEF) in SF5 denotes that it is not evident from thepublication whether the reaction channel is undefined or defined.

SF4. Reaction Product. In general, the heaviest of the products is defined as the reaction product(also called residual nucleus). In the case of two reaction products with equal mass, the one withthe larger Z is considered as the heavier product. Exceptions or special cases are:

• If SF5 contains the code SEQ, indicating that the sequence of several outgoing particlesand/or processes coded in SF3 is meaningful, the nuclide to be coded in SF4 is the heaviestof the final products.

Example: (5-B-10(N,A+T)2-HE-4,SEQ,SIG)

• Where emission cross sections, production cross sections, product yields, etc., are given forspecified nuclides, particles, or gammas, the product considered is defined as the reactionproduct (even if it is not the heaviest of several reaction products).

This subfield contains:either a blank,

Example: (26-FE-56(N,EL),,WID)or a nuclide code.

Example: (51-SB-123(N,G)51-SB-124-M1+M2/T)or, a variable nucleus codes:

Example: (92-U-235(N,F)ELEM/MASS,CUM,FY)

Quantity consists of four subfields, each separated by a comma. All combinations of codesallowed in the quantity field are given in Dictionary 36.

SF5 Branch. Indicates a partial reaction, e.g., to one of several energy levels.

SF6 Parameter. Indicates the reaction parameter given, e.g., differential cross section.

7 The code UND is presently used only for charged particle reaction data.

EXFOR Basics

B.11

SF7 Particle Considered. Indicates to which of several outgoing particles the quantity refers.8

Multiple codes, e.g., for the correlation between outgoing particles, all particles are separated bya slash.

SF8 Modifier. Contains information on the representation of the data, e.g., relative data.

Data Type Field. Indicates whether the data are experimental, theoretical, evaluated, etc. Codesare found in Dictionary 35.

Variable Nucleus. For certain processes, the data table may contain yield or production crosssections for several nuclei which are entered as variables in the data table. In this case, eitherSF1 or SF4 of the REACTION keyword contain one of the following codes:

ELEM - if the Z (charge number) of the nuclide is given in the data table.MASS - if the A (mass number) of the nuclide is given in the data table.ELEM/MASS - if the Z and A of the nuclide are given in the data table.

The nuclei are entered in the common data or data table as variables under the data headingsELEMENT and/or MASS with the units NO-DIM.

If the data headings ELEMENT and MASS are used, a third field with the data heading ISOMER

is used when isomer states are specified:0. = ground state (used only if nuclide has also an isomeric state),1. = first metastable state (or the metastable state when only one is known),2. = second metastable state, etc.

Decay data for each entry under ELEMENT/MASS(ISOMER) and their related parent or daughternuclides may be given in the usual way under the information-identifier keyword DECAY-DATA. Entries under the data headings ELEMENT/MASS(ISOMER) are linked to entries underDECAY-DATA (and RAD-DET, if present) by means of a decay flag.9

Example:

BIBREACTION (…(…,F)ELEM/MASS,…)ENDBIBNOCOMMONDATAEN ELEM MASS ISOMER DATAMEV NO-DIM NO-DIM NO-DIM B … 61. 148. 0. … … 61. 148. 1. … … 61. 149. … … 62. 149. …

8 Note that the particle considered is not necessarily identical to the particle detected, e.g., the angular distribution ofan outgoing particle which has been deduced from a recoil particle detected.9 If the half-life is the only decay data given, this may be entered in the data table under the data heading HL,although this is not recommended.

EXFOR Basics

B.12

Variable Number of Emitted Nucleons. Where mass and element distributions of productnuclei have been measured, the sum of outgoing neutrons and protons may be entered asvariables in the data table. In this case SF3 of the REACTION keyword contains at least one of thefollowing codes:

XN - variable number of neutrons given in the data table.YP - variable number of protons given in the data table.

The numerical values of the multiplicity factors X and Y are entered in the data table under thedata headings N-OUT and P-OUT, respectively.

Example:

BIBREACTION (…(…,XN+YP)…)…ENDBIBNOCOMMONDATAEN N-OUT P-OUT DATAMEV NO-DIM NO-DIM B………ENDDATA

Reaction Combinations. For experimental data sets referring to complex combinations ofmaterials and reactions, the code units defined in this section can be connected into a singlemachine-retrievable field, with appropriate separators and properly balanced parentheses. Thecomplete reaction combination is enclosed in parentheses.

The following reaction combinations are defined:

((------)+(-----)) Sum of 2 or more quantities (see LEXFOR, Sums).((------)-(-----)) Difference between 2 or more quantities.((------)*(-----)) Product of 2 or more quantities (see LEXFOR, Products).((------)/(-----)) Ratio of 2 or more quantities (see LEXFOR, Ratios).((------)//(-----)) Ratio of 2 quantities, where the numerator and denominator refer to

different values for one or more independent variables (see LEXFOR,Ratios).

((------)=(-----)) Tautologies (see LEXFOR, Tautologies for usage).

When a reaction combination contains the separator "//", the data table will contain at least oneindependent variable pair with the data heading extensions -NM and -DN.

EXFOR Basics

B.13

Example:BIBREACTION (((92-U-238(N,F)ELEM/MASS,CUM,FY,,FIS)/

(92-U-238(N,F)42-MO-99,CUM,FY,,FIS))//((92-U-235(N,F)ELEM/MASS,CUM,FY,,MXW)/(92-U-235(N,F)42-MO-99,CUM,FY,,MXW)))

RESULT (RVAL)…ENDBIBCOMMONEN-DUM-NM EN-DUM-DNMEV EV 1.0 0.0253ENDCOMMONDATAELEMENT MASS DATA…ENDDATA

REFERENCE. Gives information on references that contain information about the data coded.Other related references are not coded under this keyword (see REL-REF, MONIT-REF). Thegeneral coding format is (reference type, reference, date).

The format of the reference field is dependent on the reference type. The general format for eachreference type follows.

Type of Reference = B or C; Books and Conferences.General code format: (B or C,code,volume,(part),page(paper #),date). Codes from Dictionary 7.Examples: (C,67KHARKOV,,(56),196702) Kharkov Conference Proceedings, paper #56, February

1967. (C,66WASH,1,456,196603) Washington Conference Proceedings, Volume 1, page 456,

March 1966 (B,ABAGJAN,,123,1964) Book by Abagjan, page 123, published in 1964.

Type of Reference = J: Journals.General code format is (J,code,volume,(issue #),page,date). Codes are from Dictionary 5.Examples: (J,PR,104,1319,195612) Phys. Rev. Volume 104, page 1319, December 1956 (J,XYZ,5,(2),89,196602) Journals XYZ, Volume 5, issue #2, page 89, February 1966

Type of Reference = P or R or S; Reports.General code format: (P or R or S,code-number,date). Codes from Dictionary 6.Examples: (R,JINR-P-2713,196605) Dubna report, series P, number 2713, May 1966. (P,WASH-1068,185,196603) WASH progress report number 1068, page 185, March 1966.

EXFOR Basics

B.14

Type of Reference = T, or W; Thesis or Private Communication.General code format: (W or T,author,page,date)Examples: (W,BENZI,19661104) private communication from Benzi, November 4, 1966. (T,ANONYMOUS,58,196802) thesis by Anonymous, page 58, February 1968.

REL-REF. Gives information on references related to, but not directly pertaining to, the workcoded. The general code format is: (code,subaccession#,author,reference).

Code: code from Dictionary 17.

Subaccession #: EXFOR subaccession number for the reference given, if it exists.Cnnnn001 refers to the entire entry Cnnnn. Cnnnn000 refers to a yet unassigned subentrywithin the entry Cnnnn.

Author: first author, coded as under AUTHOR, followed by + when more than one authorexists.

Reference: coded as for REFERENCE.

Example:

(C,B9999001,A.B.NAME+,J,XYZ,5,(2),90,197701) Critical remarks by A.B.Name, et al.,in journal XYZ, volume 5, issue #2, p. 90, January 1977.

RESULT. Describes commonly used quantities that are coded as REACTION combinations.

Example: REACTION ((Z-S-A(N,F)ELEM/MASS,CUM,FY)/(Z-S-A(N,F)MASS,CHN,FY))

RESULT (FRCUM)

SAMPLE. Used to give information on the structure, composition, shape, etc., of themeasurement sample.

STATUS. Givews information on the status of the data presented. Entered in one of the generalcode formats, or for cross reference to another data set, the general code format is:(code,subaccession#)

Code: code from Dictionary 16.

• Subaccession# Field: cross-reference to an EXFOR subaccession number, see REL-REF.

Example:STATUS (SPSDD,10048009) - this subentry is superseded by subentry 10048009.

TITLE. Gives the title for the work referenced.

EXFOR Basics

C.1

Appendix C

COVARIANCE DATA FILE FORMAT

Where covariance files are large, the covariance data may be stored in a separate covariance file.The existance of the file will be indicated in the corresponding EXFOR data set under theinformation-identifier keyword COVARIANCE, see Appendix B, COVARIANCE.

There are three record types in the covariance file:• comment records,• data records,• end records.

Comment record formatColumn 1 C

2 – 9 Data set number (subaccession number)10 (blank)11 - 80 Comment which includes covariance type and format

Data record formatColumn 1 D

2 - 9 Data set number (subaccession number)10 (blank)11 - 80 Data in format given on comment record

End record formatColumn 1 E

2 - 9 Data set number (subaccession number)10 - 80 (blank)

EXFOR Basics

EXFOR Basics

D.1

Appendix D

Table of Dictionaries

The EXFOR System Dictionaries list all keywords and codes used in the EXFOR entries.Listings are included for the following dictionaries. Where the dictionary is large, the most usedcodes are given. A complete listing of all dictionaries and codes is available from any of theNuclear Reaction Data Centers.

Page

Dictionary 3. Institutes............................................................................................. D.3

Dictionary 4. Reference Type.................................................................................. D.7

Dictionary 5. Journals .............................................................................................. D.7

Dictionary 7. Conference and Books..................................................................... D.10

Dictionary 15. History ........................................................................................... D.12

Dictionary 16. Status.............................................................................................. D.13

Dictionary 17. Rel-Ref........................................................................................... D.13

Dictionary 18. Facility ........................................................................................... D.14

Dictionary 19. Incident Source .............................................................................. D.15

Dictionary 20. Additional Results ......................................................................... D.16

Dictionary 21. Method........................................................................................... D.17

Dictionary 22. Detectors ........................................................................................ D.19

Dictionary 23. Analysis ......................................................................................... D.20

Dictionary 24. Data Headings................................................................................ D.21

Dictionary 30. Process ........................................................................................... D.22

Dictionary 33. Particles ......................................................................................... D.23

Dictionary 34. Modifiers (REACTION SF8) ........................................................ D.24

Dictionary 35. Data-Type (REACTION SF9)....................................................... D.25

Dictionary 36. Quantities (REACTION SF5-7) .................................................... D.26

Dictionary 37. Result ............................................................................................. D.30

EXFOR Basics

D.2

EXFOR Basics

D.3

Dictionary 3. Institutes: used with the keywords INSTITUTE and FACILITY. The firstcharacter of the codes designates the area of responsibility (see Appendix A), the next threecharacters designate the country, and the last three characters specify the institute. A subsetcontaining some of the most frequently used codes is given here.

Area 1: United States and CanadaCanada

1CANCRC A.E.C.L., Chalk River, Ontario1CANMCM McMaster University, Hamilton, Ontario1CANTMF Tri University Meson Facility, Vancouver, B.C.

United States1USAANL Argonne National Laboratory, Argonne, IL1USAARK Univ. of Arkansas, Fayetteville, AR1USABNL Brookhaven National Laboratory, Upton, NY1USABNW Pacific Northwest Laboratories, Richland, WA1USABRK Univ. of Calif. Lawrence Berkeley Lab., Berkeley, CA1USACOL Columbia University, New York, NY1USADAV University of California, Davis, CA1USADKE Duke University, Durham, NC1USAFSU Florida State University, Tallahasse, FL1USAGEO University of Georgia, Athens, GA1USAGGA Gulf General Atomic, San Diego, CA1USAGIT Georgia Institiute of Technology, Atlanta, GA1USAHAN Hanford Atomic Products, Richland, WA1USAINL Idaho Nuclear Engineering Lab., Idaho Falls, ID1USAINU Indiana University, Bloomington, IN1USAKAP Knolls Atomic Power Laboratory, Schenectady, NY1USAKTY University of Kentucky, Lexington, KY1USALAS Los Alamos National Laboratory, NM1USALRL Lawrence Livermore National Laboratory, Livermore, CA1USALTI University of Lowell, Lowell, MA1USAMHG University of Michigan, Ann Arbor, MI1USAMIT Massachusetts Institute of Technology, Cambridge, MA1USAMRY University of Maryland, College Park, MD1USANBS National Bureau of Standards, Washington, DC1USANIS National Inst.of Standards & Techn., Gaithersburg, MD1USANOT Univ. of Notre Dame, Notre Dame, IN1USAOHO Ohio University, Athens, OH1USAORL Oak Ridge National Laboratory, Oak Ridge, TN1USARPI Rensselaer Polytechnic Institute, Troy, NY1USATEX Univ. of Texas, Austin, TX1USATNL Triangle Universities Nuclear Lab., Durham, NC1USAWIS University of Wisconsin, Madison, WI

EXFOR Basics

D.4

Area 2: OECD CountriesAustria

2AUSIRK Inst. fuer Radiumforschung und Kernphysik, ViennaBelgium

2BLGMOL C.E.N., MolDenmark

2DENRIS Riso, RoskildeFinland

2SF JYV Jyvaeskylae Univ., JyvaeskylaeFrance

2FR BRC CEN Bruyere-le-Chatel2FR CAD C.E.N. Cadarache2FR FAR CEA Fontenay-aux-Roses, Seine2FR GRE Grenoble, Isere, (CEA and Univ.)2FR PAR Univ. of Paris, (incl.Orsay), Paris2FR SAC C.E.N. Saclay

Germany2GERFRK J.W.Goethe Univ.,Frankfurt2GERGSI Gesellschaft fuer Schwerionenforschung, Darmstadt2GERHAM Hamburg, Universitaet2GERJUL Kernforschungsanlage Juelich2GERKFK Kernforschungszentrum, Karlsruhe2GERKIL Univ. of Kiel, Kiel2GERMUN Technische Universitaet Muenchen2GERPTB Phys.Techn.Bundesanst., Braunschweig2GERZFK Zentralinst.f.Kernforschung, Rossendorf

Greece2GRCATH CNRC Demokritos, Athens

Italy2ITYBOL ENEA Centro Ricerche Energia di Bologna2ITYCAT Univ. of Catania2ITYPAD Padua, University and Lab. Nat. Legnaro

Japan2JPNJAE JAERI, Tokai2JPNKTO Kyoto Univ., Kyoto2JPNKYU Kyushu Univ., Dept.of Nucl.Eng., Fukuoka2JPNOSA Osaka Univ., Osaka2JPNTIT Tokyo Inst.of Technology, Tokyo2JPNTOH Tohoku Univ., Sendai2JPNTOK Tokyo Univ., Tokyo

The Netherlands2NEDGRN Groningen2NEDRCN Netherland’s Energy Research Foundation, Petten

Norway2NORKJL Inst. foer Atomenergi, Kjeller

EXFOR Basics

D.5

Sweden2SWDAE Studsvik Energiteknik AB2SWDFOA Research Inst. for National Defence, Stockholm

Switzerland2SWTETH Eidgenossische Technische Hochschule, Zuerich2SWTPSI Paul Scherrer Inst., Villigen

United Kingdom2UK ALD Awre, Aldermaston, England2UK DOU Dounreay Experimental Reactor Establishment, England2UK HAR AERE, Harwell, Berks, England2UK NPL National Phys.Lab., Teddington, England2UK OXF Univ. of Oxford, Oxford, England

Area 3: Remaining countries outside other 3 areasAustralia

3AULAML Univ. of Melbourne, Melbourne3AULAUA Australian Nucl. Sci. and Techn.Org., Lucas Heights, SW3AULCBR Australian National Univ., Canberra

China3CPRAEP Inst. of Atomic Energy, Beijing3CPRBJG Beijing Univ., Beijing3CPRLNZ Lanzhou Univ., Lanzhou3CPRNIX Northwest Inst.of Nucl.Technology, Xian3CPRNRS Inst.of Nucl.Research, Acad.Sinica, Shanghai3CPRSST Shanghai Univ. of Science and Technology3CPRTSI Tsinghua Univ., Beijing

Croatia3CRORBZ Inst.Rudjer Boskovic, Zagreb3CROZAG Univ. of Zagreb, Zagreb

Czechoslovakia3CZRUJV Inst. of Nuclear Research, Rez i Prahy

Hungary3HUNDEB Inst.of Nuclear Research, ATOMKI, Debrecen3HUNKFI Central Research Inst. for Physics, KFKI, Budapest3HUNKOS Inst. for Experimental Physics, Kossuth U., Debrecen

India3INDBOS Bose Institute, Calcutta3INDMUA Muslim Univ., Aligarh3INDSAH Saha Institute, Calcutta3INDTAT Tata Institute, Bombay3INDTRM Bhabha Atom.Res.Centre, Trombay

Israel3ISLNEG Ben Gurion Univ. of the Negev, Beer-Sheva3ISLWEI Weizmann Inst., Rehovoth

EXFOR Basics

D.6

Mexico3MEXUMX Univ. Nacionale Autonoma de Mexico, Mexico City

New Zealand3NZLNZH Inst.of Nuclear Sciences, Lower Hutt

Poland3POLIPJ Soltan Inst.Probl.Jadr., Swierk+Warszawa3POLWWA Warszawa, University

Romania3RUMBUC Inst. de Fizica si Inginerie Nucleara, Bucharest

South Africa3SAFPEL Atomic Energy Corp.of South Africa, Pelindaba

Area 4: Countries of the former Soviet UnionArmenia

4ARMJER Inst. Fiziki Armenian A.N., JerevanBelorus

4BLRIJE Inst. Yad. Energetiki A.N.Byeloruss.SSR, MinskKazakhstan

4KASKAZ Inst.Yadernoi Fiziki, Alma-AtaLatvia

4LATIFL Inst. Fiziki Latviyskoi A.N., RigaRussia

4RUSEPA Experimental Physics Inst., Arzamas4RUSFEI Fiziko-Energeticheskii Inst., Obninsk4RUSFTI Fiz.-Tekhnicheskiy Inst.Ioffe, St.Petersburg+Gatchina4RUSICP Inst.of Chemical Phys., Moscow4RUSITE Inst.Teoret.+ Experiment. Fiziki, Moscow4RUSJIA Inst.Yadernych Issledovaniy Russian Acad. Sci.4RUSKUR Inst.At.En. I.V.Kurchatova, Moscow4RUSLEB Fiz.Inst. Lebedev (FIAN), Moscow4RUSLIN Leningrad Inst.Nucl.Phys., Russian Acad.Sci., Gatchina4RUSMOS Moscow State Univ., Nuclear Physics Inst., Moscow4RUSNIR NIIAR Dimitrovgrad4RUSRI Khlopin Radiev.Inst., Leningrad

Ukraine4UKRIJI Inst. Yadernykh Issledovaniy Acad. Sct. Ukraine, Kiev4UKRKFT Kharkovskii Fiziko-Tekhnicheskii Inst., Kharkov4UKRKGU Gosudarstvennyi Univ.(State Univ.), Kiev

International4ZZZDUB Joint Inst.for Nucl.Res., Dubna

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Dictionary 4: Reference type: used as the first subfield for the keyword REFERENCE, and,similarly, for MONIT-REF, and REL-REF.

B BookC ConferenceJ JournalP Progress reportR Report other than progress reportS Report containing conference proceedingsT Thesis or dissertationW Private communication

Dictionary 5: Journal codes: used as the second subfield for the keyword REFERENCE, whenthe reference type is given as J; similarly, for MONIT-REF, and REL-REF. A subset containingsome of the most frequently used codes is given here. The code may have an extensiondelimited by a slash; these extensions have the following meanings:

/A, /B,..., /G section or series/L letters section/S supplement

ACR Acta CrystallographicaADP Annalen der PhysikAE Atomnaya EnergiyaAEJ Journal of the Atomic Energy Society of JapanAF Arkiv foer FysikAHP Acta Physica HungaricaAJ Astrophysical JournalAK Atomki KozlemenyekAKE AtomkernenergieANP Annalen der Physik (Leipzig)ANS Transactions of the American Nuclear SocietyAP Annals of Physics (New York)APA Acta Physica AustriacaAPP Acta Physica PolonicaARI Applied Radiation and IsotopesAUJ Australian Journal of PhysicsBAP Bulletin of the American Physical SocietyBAS Bull.Russian Academy of Sciences - PhysicsCHP Chinese Journal of Physics (Taiwan)CJP Canadian Journal of PhysicsCR Comptes RendusCZJ Czechoslovak Journal of PhysicsDOK Doklady Akademii NaukEPJ European Physics JournalFIZ Fizika

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HPA Helvetica Physica ActaIJP Indian Journal of PhysicsINC Inorganic and Nuclear Chemistry LettersISP Israel J.of PhysicsIZV Izv.Rossiiskoi Akademii Nauk,Ser.Fiz.JAE Yadernaya EnergetikaJEL Soviet Physics - JETP LettersJET Soviet Physics - JETPJIN Journal of Inorganic and Nuclear ChemistryJNE Journal of Nuclear EnergyJP Jour. of PhysicsJPJ Journal of the Physical Society of JapanJPR Journal de Physique (Paris)JRC J.of Radioanalytical ChemistryJRN J.of Radioanalytical and Nuclear ChemistryKFI KFKI KozlemenyekNC Nuovo CimentoNCL Lettere al Nuovo CimentoNCR Rivista del Nuovo CimentoNCS Nuovo Cimento, Suppl.NIM Nuclear Instrum.and Methods in Physics Res.NKA NukleonikaNP Nuclear PhysicsNSE Nuclear Science and EngineeringNST J.of Nuclear Science and Technology, TokyoNWS NaturwissenschaftenPAN Physics of Atomic NucleiPCJ Journal of Physical ChemistryPHE High Energy Physics and Nucl.Physics,Chinese ed.PHY Physica (Utrecht)PL Physics LettersPNE Progress in Nuclear EnergyPPS Proceedings of the Physical Society (London)PR Physical ReviewPRL Physical Review LettersPRS Proc. of the Royal Society (London)PS Physica ScriptaPTE Pribory i Tekhnika EksperimentaRCA Radiochimica ActaRJP Romanian Journal of PhysicsRRL Radiochem.and Radioanal.LettersRRP Revue Roumaine de PhysiqueSJA Soviet Atomic EnergySJPN Soviet Journal of Particles and NucleiSPC Soviet Physics-Cristallography

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SPD Soviet Physics-DokladyUFZ Ukrainskii Fizichnii ZhurnalUPJ Ukrainian Physics JournalYF Yadernaya FizikaYK Vop. At.Nauki i Tekhn.,Ser.Yadernye KonstantyZEP Zhurnal Eksper. i Teoret. Fiz., Pisma v Redakt.ZET Zhurnal Eksperimental’noi i Teoret. FizikiZP Zeitschrift fuer Physik

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Dictionary 7: Books and Conferences: used as the second subfield for the keyword REFERENCE,when the reference type is given as B or C, and similarly, for MONIT-REF, and REL-REF. A subsetcontaining some of the most frequently used codes is given here.

BooksACT.EL Actinide ElementsEXP.NUC.P. Experimental Nuclear PhysicsFAST N.PH. Fast Neutron PhysicsNB.GS.COMP Noble Gas Compounds, Chicago Press 1963NEJTRONFIZ Neitronnaya Fizika, Moskva 1961PR.NUC.EN. Progress in Nucl.EnergyRCS Radiochemical Studies, Fission ProductsSPN Sov.Progr.in Neutr.Phys.,New York 1961TRANSU.EL. Transuranium Elements

Conferences55GENEVA 1st Conf. on Peaceful Uses Atomic Energy, Geneva 195555MOSCOW USSR Conf. Peaceful Uses of Atomic Energy, Moscow 195556KIEV Kiev Conf., Kiev 195658GENEVA 2nd Conf. on Peaceful Uses Atomic Energy, Geneva 195858PARIS Nuclear Physics Congress, Paris 195859CALCUTTA Low Energy Nuclear Physics Symp., Calcutta 195959LONDON Conf.Nuclear Forces and Few-Nucleon Problem, London 195960BASEL Conf. on Polarization Phenom. in Nuclear Reactions, Basel 196060VIENNA Pile Neutron Research Symp., Vienna 196060WIEN Neutron Inelastic Scattering Symp., Vienna 196061BOMBAY Nuclear Physics Symp., Bombay 196161BRUSSELS Neutron Time-of-Flight Colloquium, Brussels 196161DUBNA Slow Neutron Physics Conf., Dubna 196161MANCH Rutherford Conf., Manchester 196161RPI Neutron Physics Symp., Rensselaer Polytech 196161SACLAY Time of Flight Methods Conf., Saclay 196162PADUA Nucl. Reaction Mechanisms Conf., Padua 196263BOMBAY Nuclear and Solid State Physics Symp., Bombay 196363KRLSRH Neutron Physics Conf., Karlsruhe 196364BOMBAY Neutron Inelastic Scattering Symp., Bombay 196464GENEVA 3rd Conf. on Peaceful Uses Atomic Energy, Geneva 196464PARIS Nuclear Physics Congress, Paris 196465CALCUTTA Nuclear and Solid State Phys.Symp., Calcutta 196565KRLSRH Pulsed Neutron Symp., Karlsruhe 196565SALZBURG Physics and Chemistry of Fission Conf., Salzburg 196566BOMBAY Nuclear and Solid State Physics Symp., Bombay 196666GATLNBG Int. Conf. on Nuclear Physics, Gatlinburg, 196666MOSCOW Nuclear Spectroscopy Conf., Moscow 196666PARIS Nuclear Data For Reactors Conf., Paris 1966

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66WASH Neutron Cross-Section Technology Conf., Washington 196667BRELA Light Nuclei Symp., Brela 196767JUELICH Neutron Physics at Reactors Conf., Juelich 196767KARLSR Symp. on Fast Reactor Physics,Karlsruhe 196768BOMBAY Nuclear and Solid State Physics Symp., Bombay 196868COPENHGN Neutron Inelastic Scattering Symp., Copenhagen 196868MADRAS Nuclear and Solid State Physics Symp., Madras 196868WASH Nuclear Cross-Sections & Technology Conf., Washington 196869ROORKEE Nuclear and Solid State Physics Symp., Roorkee 196969VIENNA Physics and Chemistry of Fission Symp., Vienna 196970ANL Neutron Standards Symp., Argonne 197070HELSINKI Nuclear Data for Reactors Conf., Helsinki 197070MADISON Polarization Phenomena Conf., Madison 197070MADURAI Nuclear and Solid State Physics Symp., Madurai 197071KIEV Neutron Physics Conf., Kiev 197171KNOX Conf. Neutron Cross Sections & Techology, Knoxville 197172BOMBAY Nuclear and Solid State Physics Symp, Bombay 197272GRENOBLE Neutron Inelastic Scattering Symp., Grenoble 197272KIEV Nuclear Spectroscopy Conf, Kiev 197273BANGLO Nuclear and Solid State Physics Symp.,Bangalore,197373KIEV Conf.on Neutron Physics, Kiev 197373MUNICH Conf. on Nuclear Physics,Munich 197373PACIFI Conf. on Photonuclear Reactions, Pacific Grove 197373PARIS Applications of Nuclear Data Symp., Paris 197374BOMBAY Nuclear and Solid State Physics Symp., Bombay 197474PETTEN Symp. on Neutron Capture Gamma Ray Spectroscopy, Petten 197475CALCUTTA Nuclear and Solid State Physics Symp.,Calcutta,197575KIEV Conf. on Neutron Phys., Kiev 197575WASH Conf. on Nuclear Cross Sections and Technology, Washington 197575ZURICH Symp. on Polarization Phenomena, Zuerich 197576AHMEDABA Nuclear Physics & Solid State Physics Symp., Ahmedabad,197676LOWELL Conf. on Interaction of Neutrons with Nuclei, Lowell 197677BNL Symp. on Neutron Cross Sections at 10 - 40 Mev, Brookhaven 197777KIEV Conf. on Neutron Physics, Kiev 197777NBS Symp.on Neutron Standards, Gaithersburg 197777VIENNA Symp. on Neutron Inelastic Scattering, Vienna 197778BNL Symp. on Neutron Capture Gamma Ray Spectroscopy, Brookhaven 197878BOMBAY Nuclear Physics and Solid State Physics Symp., Bombay 197878HARWELL Conf. on Neutron Physics and Nuclear Data, Harwell 197879JUELICH Symp. on Physics and Chemistry of Fission, Juelich 197979KNOX Conf. on Nuclear Cross Sections fro Technology, Knoxville 197979MADRAS Nuclear Physics and Solid State Physics Symp., Madras 197979SMOLENIC Symp. on Neutron Induced Reactions, Smolenice 197980BERKELEY Conf. on Nuclear Physics, Berkeley 198080BNL Symp. on Neutron Cross Sections at 10-50 MeV, Brookhaven 1980

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80KIEV All-Union Conf. on Neutron Physics, Kiev 198080SANTA FE Symp. on Polarization Phenomena in Nuclear Physics, Santa Fe 198081ANL Neutron Scattering Conf., Argonne 198181BOMBAY Nuclear Physics and Solid State Physics .Symp., Bombay 198181GRENOB Symp. on Neutron Capture Gamma-Ray Spectroscopy, Grenoble 198182ANTWER Conf. on Nuclear Data for Science and Technology, Antwerp 198282SMOLEN Conf. on Neutron Induced Reactions, Smolenice 198283KIEV All-Union Conf. on Neutron Physics, Kiev 198383MYSORE Nuclear Physics and Solid State Physics Symp., Mysore 198384GAUSSIG Symp. on Nuclear Physics, Gaussig 198484KNOX Symp. on Capture Gamma Ray Spectroscopy, Knoxville 198485JUELIC Conf. on Neutron Scattering in the Nineties, Juelich 198585SANTA Conf.on Nuclesar Data for Basic and Applied Science, Santa Fe 198586DUBROV Conf. on Fast Neutron Phys., Dubrovnik 198686HARROG Nuclear Physics Conf., Harrogate 198687KIEV Conf. on Neutron Physics, Kiev 198788BOMBAY Nuclear Physics Symp., Bombay 198888MITO Conf. on Nuclear Data for Science and Technology, Mito 198889LENING 50th Anniversary of Nuclear Fission, Leningrad 198989WASH 50 Years of Nuclear Fission, Washington D.C. 198991BEIJIN Symp. on Fast Neutron Physics, Beijing 199191JUELIC Conf. on Nuclear Data for Science and Technology, Juelich 199192BOMBAY Nuclear Physics Symp., Bombay 199294GATLIN Nuclear Data for Science & Technology, Gatlinburg 199496BUDA Symp. on Capture Gamma Ray Spectroscopy, Budapest, 199696NOTRED Nuclei in the Cosmos IV, Notre Dame, IN, 199697TRIEST Nuclear Data for Science & Technology, Trieste, Italy, 199798VOLOS Nuclei in the Cosmos V, Volos, Greece, 1998

Dictionary 15: History codes:: used with the keyword HISTORY.

A Important alterationsC Complied at the data centerD Entry or subentry deletedE Transmitted to other data centersL Entered into data libraryR Data received at the data centerT Converted from previous compilationU Unimportant alterations

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Dictionary 16: Status codes: used with the keyword STATUS.

APRVD Approved by authorCOREL Data correlated with another data setCPX Data taken from data file of McGowan, et al.CURVE Data read from a curveDEP Dependent dataNCHKD Original reference not checkedNDD Data converted from NEUDADA fileOUTDT Normalization out-of-datePRELM Preliminary dataRIDER Data converted from file of B.F. RiderRNORM Data renormalized by other than authorSCSRS Data converted from SCISRS fileSPSDD Data supersededTABLE Data received by center in tabular formUNOBT Data unobtainable from author

Dictionary 17: Related Reference codes: used with the keyword REL-REF.

A Reference with which data agreeC Critical remarksD Reference with which data disagreeE Reference used in the evaluationN -R Reference from which data were used

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Dictionary 18: Facility codes: used with the keyword FACILITY.

ACCEL AcceleratorBETAT BetatronCCW Cockcroft-Walton acceleratorCHOPF Fast chopperCHOPS Slow chopperCYCLO CyclotronCYCTM Tandem cyclotronsCYGFF CyclograaffDYNAM DynamitronESTRG Electron storage ringICTR Insulated core transformer acceleratorISOCY Isochronous cyclotronLINAC Linear acceleratorMESON Meson facilityMICRT MicrotronOLMS On-line mass separatorOSCIP Pile oscillatorREAC ReactorSELVE Velocity selectorSPECC Crystal spectrometerSPECD Double mass spectrometerSPECM Mass spectrometerSYNCH SynchrotronSYNCY SynchrocyclotronVDG Van de GraaffVDGT Tandem Van de Graaff

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Dictionary 19: Incident Source codes: used with the keyword INC-SOURCE.

A-BE Alpha-BerylliumARAD Annihilation radiationATOMI Atomic beam sourceBRST BremsstrahlungCF252 Spontaneous fission of 252CfCM244 Spontaneous fission of 244CmCM246 Spontaneous fission of 246CmCM248 Spontaneous fission of 248CmCOMPT Compton scatteringD-BE Deuteron-BerylliumD-C12 Deuteron-12CD-C14 Deuteron-14CD-D Deuteron-DeuteriumD-LI Deuteron-LithiumD-LI7 Deuteron-7LiD-N15 Deuteron-15ND-T Deuteron-TritiumEVAP Evaporation neutronsEXPLO Nuclear explosive deviceHARD HardenedKINDT Kinematically determinedLAMB Lamb-shift sourceLASER Laser scatteringMPH Monoenergetic photonsP-BE Proton-BerylliumP-D Proton-DeuteriumP-LI7 Proton-7LiP-T Proton-TritiumPHOTO Photo-neutronPOLIS Polarized ion sourcePOLNS Polarized neutron sourcePOLTR Polarized targetPU240 Spont.fission of 240PuQMPH Quasi-monoenergetic photonsREAC ReactorSPALL SpallationTAGD Electron taggedTHCOL Thermal columnTHRDT Determined by threshold techniqueVPH Virtual photons

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Dictionary 20: Additional Result Codes: used with the keyword ADD-RES.

A-DIS Mass distributionAMFF Angular momentum of fission fragmentsANGD Angular distributionCOMP Comparison with calculated valuesDECAY Decay properties investigatedE-DIS Energy distributionG-SPC Gamma spectraLD Level densityN-SPEC Neutron spectraP-SPEC Proton spectraPOT Parameters of nuclear potentialRANGE Range of recoils measuredRECIP Reciprocal dataSTRUC Nuclear structure dataTHEO TheoryTRCS Total reaction cross sectionTTY-C Calculated thick target yieldZ-DIS Charge distribution

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Dictionary 21: Method Codes: used with the keyword METHOD.

ABSFY Absolute fission yield measurementACTIV ActivationAMS Accelerator mass spectrometryASEP Separation by mass separatorASSOP Associated particleBCINT Beam current integratedBGCT ß-? coincidence techniqueBSPEC ß-ray spectrometryBURN Burn-upCADMB Cadmium bathCHRFL Christiansen filterCHSEP Chemical separationCOINC CoincidenceDIFFR DiffractionDSCAT Double scatteringEDE Particle identification by ‘E/∆E’ measurementEDEG Energy degradation by foilsEXTB Irradiation with external beamFISCT Absolute fission countingFLUX Neutron flux monitoringFPGAM Direct ?-ray spectrometryGSPEC γ- ray spectrometryHADT Heavy atom difference techniqueHATOM Hot atom methodHEJET Collection by He jetINTB Irradiation with internal beamJET Collection by gas jetLRASY Left-right asymmetryMAGFR Magnetic field rotationMANGB Manganese bathMASSP Mass spectrometryMOMIX Mixed monitorMOSEP Separate monitor foilOLMS On-line mass separationPHD Pulse-height discriminationPLSED Pulse die-awayPSD Pulse-shape discriminationRCHEM Radiochemical separationREAC Reactivity measurementREC Collection of recoilsREFL Total reflection from mirrorsRELFY Relative fission yield measurementRVAL R-value measurementSFLIP Spin flip

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SHELT Shell transmissionSITA Single target irradiationSLODT Slowing-down timeSTATD Statistically determinedSTTA Stacked target irradiationTOF Time-of-flight

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Dictionary 22: Detector Codes: used with the keyword DETECTOR.

BF3 BF3 neutron detectorBGO Bismuth-germanate crystal detectorBPAIR Electron-pair spectrometerCEREN Cerenkov detectorCOIN Coincidence counter arrangementCSICR Cesium-Iodide crystalD4PI 4p detectorFISCH Fission chamberGE-IN Germanium intrinsic detectorGELI Ge(Li) detectorGEMUC Geiger-Mueller counterGLASD Glass detectorHE3SP 3He spectrometerHORBU Hornyak button detectorHPGE Hyperpure Germanium detectorIOCH Ionization chamberLONGC Long counterMAGSP Magnetic spectrometerMOXR Moxon-Rae detectorMTANK Moderating tank detectorMWPC Position sensitive multi-wire proportional counterNAICR NaI(Tl) crystalPLATE Nuclear platesPROPC Proportional counterPSSCN Position sensitive scintillatorPSSSD Position sensitive solid state detectorSCIN Scintillation detectorSILI Si(Li) detectorSOLST Solid-state detectorSTANK Scintillator tankSWPC Position sensitive single-wire proportional counterTELES Counter telescopeTHRES Threshold detectorTRD Track detector

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Dictionary 23: Analysis Codes: used under the keyword ANALYSIS.

4PI1A 4p times differential cross section at one angleAREA Area analysisCORAB Correction for isotopic abundanceDECAY Decay curve analysisDIFFR Difference spectrumDTBAL Detailed balanceINTAD Integration of angular distributionINTED Integration of energy distributionLEAST Least-structure methodMLA Multilevel analysisPHDIF Photon differencePLA Penfold-Leiss methodREDUC Reduction methodREGUL Regularization methodRFN R-function formalismSHAPE Shape analysisSLA Single level analysisTHIES Thies’s methodUNFLD Unfolding procedureWSP Woods-Saxon potential

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Dictionary 24: Data Headings: used at the beginning of the COMMON and DATA fields toindicate the significance of the variable given; also used under the keywords ASSUMED,MONITOR, HALF-LIFE, MISC, and ERR-ANALYS as links to the data field.The codes given in this dictionary may be followed by one of the following suffixes.

-1, -2, etc. 1st, 2nd, etc., value, when more than one defined-APRX value is approximate-CM value is in center-of-mass (quantities without this suffix are in the laboratory

system-DN value for denominator of a reaction ratio-ERR uncertainty on value-MIN minimum value-MAX maximum value-MEAN mean value-NM value for numerator of a reaction ratio-NRM value at which data is normalized-RSL resolution of value

ANAL-STEP Analysis energy stepANG AngleASSUM Assumed value, defined under ASSUMEDCOS Cosine of angleDATA Value of quantity Specified under REACTIONDECAY-FLAG Decay flag. link to information under DECAY-DATAE Energy of outgoing particleE-DGD Degradation in secondary particle energy vs. incident energyE-EXC Excitation energyE-GAIN Gain in secondary particle energy vs. incident energyE-LVL Level energyE-LVL-FIN Final level of ? transitionE-LVL-INI Initial level of ? transitionELEMENT Atomic number of elementEMS Effective mass squaredEN Energy of incident projectileEN-DUMMY Dummy incident projectile energy, for broad spectrumEN-RES Resonance energyEN-RSL-FW Incident projectile energy resolution (FWHM)EN-RSL-HW Incident projectile energy resolution (?? FWHM)ERR Systematic uncertainty, defined under ERR-ANALYSERR-S Statistical uncertainty (1 s)ERR-T Total uncertainty (1 s)FLAG Flag, link to information under FLAGHL Half-life of nuclide specifiedISOMER Isomeric state for nuclide givenKT Spectrum temperatureLVL-FLAG Level flag, link to information under LEVEL-PROPLVL-NUMB Level number

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MASS Atomic mass of nuclideMASS-RATIO Ratio of atomic masses of fission fragmentsMISC Miscellaneous information, defined under MISC-COLMOM Linear momentum of incident projectileMOM-SEC Linear momentum of outgoing particleMOMENTUM L Angular momentum (l) of resonanceMONIT Normalization value, for reaction given under MONITORMSS-T Transverse mass of outgoing projectile (relativistic data)MSS-TK Transverse mass minus rest mass of outgoing projectile (relativistic data)MU-ADLER µ (for Adler-Adler resonance parameters)N-OUT Number of emitted neutrons, for variable number of nucleons in reactionNUMBER Fitting coefficient numberP-OUT Number of emitted protons, for variable number of nucleons in reactionPARITY Parity (p) of resonancePOL-BM Beam polarizationPOL-TR Target polarizationPOLAR PolarityQ-VAL Q-valueRAP Rapidity (relativistic data, function of (energy+mom(?))/(energy-mom(?))RAP-PS Pseudo rapidity (relativistic data, function of (mon+mom(?))/(mon-mom(?))SPIN J Spin (J) of resonanceSTAT-W G Statistical-weight factor (g)TEMP Sample temperatureTHICKNESS Sample thickness

Dictionary 30: Process Codes: used in REACTION subfield 3, and simarly under ASSUMED andMONITOR.

ABS AbsorptionEL Elastic scatteringF FissionINL Inelastic scatteringNON Nonelastic (= total minus elastic)PAI Pair production (for photonuclear reactions)SCT Total scattering (elastic + inelastic)THS Thermal neutron scatteringTOT TotalX Process unspecifiedXN Variable number of emitted neutronsYP Variable number of emitted protons

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Dictionary 33: Particle Codes: used in REACTION quantity subfields 2, 3, 7, and simarly underASSUMED and MONITOR. Also used under the keywords DECAY-DATA, DECAY-MON, PART-DET

and RAD-DET, and as the second field under the keywords EN-SEC, EMS-SEC, and MOM-SEC.

0 (no outgoing particles)A a particlesAR Annihilation radiationB Decay βB+ Decay β+B- Decay β-D DeuteronsDG Decay γDN Delayed neutronsE ElectronsEC Electron captureFF Fission fragmentsG γHE3 3HeHE6 6HeHF Heavy fragmentICE Internal-conversion electronsLCP Light charged particle (Z<7)LF Light fragmentN NeutronsP ProtonsPI π, unspecifiedPIN π-PIP π+PN Prompt neutronsRCL Recoil nucleusRSD Residual nucleusSF Fragments from spontaneous fissionT TritonsXR X-rays

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Dictionary 34: Modifier Codes: used in REACTION the 4th quantity subfield (REACTION SF8),and similarly, under ASSUMED and MONITOR.

(A) uncertain if corrected for natural isotopic abundance1K2 form: k2 dσ/dΩ = Σ (a(L)*p(L))2AG times 2 * isotopic abundance and statistical weight factor2G times 2 * staistical weight factor2L2 form: dσ/dΩ = 1/2 Σ (2L+1)*a(L)*p(L)2MT times 2p * transverse secondary mass2PT times 2p* transverse secondary momentum4AG times 4 * isotopic abundance and statistical weight factor4PI times 4πA times natural isotopic abundanceAA Adler-Adler formalismAG times isotopic abundance and statistical weight factorAL1 Associated Legendre polynomials of the first kindANA analyzing powerASY asymmetry of polarization of outgoing particlesAV averageAYY spin-correlation function, spins normal to scattering planeBRA Bremsstrahlung spectrum averageBRS average over part of Bremsstrahlung spectrumCOS Cosine coefficientsCS2 form: a0 + a1*sin2 + a2*sin2*cos + a3*sin2*cos2

EPI epi-thermal neutron spectrum averageFCT times a factor (see text)FIS fission spectrum averageFST fast reactor neutron spectrum averageG times statistical weight factorL4P form: 4π ds/dΩ = Σ (2L+1)*a(L)*p(L)LEG Legendre coefficientsLIM given for a limited energy rangeMSC approximate definition only (see text)MXW Maxwellian averagePP Incident projectile parallel/perpendicular to reaction planeRAT ratioRAW raw data (see text)REL relative dataRES at peak of resonanceRM Reich-Moore formalismRMT R-matrix formalismRNV non-1/v partRS times 4π/σRS0 (dσ/dΩ)/(dσ/dΩ at 0°) = Σ a(L)*p(L)RSD relative to 90° dataRSL form: (4p/σ)*(dσ/dΩ) = Σ (2L+1)*a(L)*p(L)

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RTE times square-root(E)RTH relative to Rutherford scatteringRV 1/v part onlyS0 times total peak cross sectionS2T form: dσ/dΩ = a0 + a1*sin2(T) + a2*sin2(2*T)SN2 sum in the power of sin2

SPA spectrum averageSQ quantity squaredSS spin-spinSUM sumTT measured for thick targetVGT Vogt formalism

Dictionary 35: Data Type Codes: used in REACTION subfield 9.

CALC Calculated dataDERIV Derived dataEVAL Evaluated dataEXP Experimental dataRECOM Recommended data

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Dictionary 36: Quantity Codes: used for quantity (REACTION subfields 5-7), and simarlarlyunder ASSUMED and MONITOR. They may be combined with modifer codes from Dictionary 34to form the complete quantity string. The code * in the 3rd field (SF7) signifies that any particlecode from Dictionary 33 given in place of the character.

The following branch codes may appear at the beginning of the string:CUM cumulative(CUM) uncertain if reaction is cumulativeM+ including decay from metastable stateM- excluding decay from metastable state(M) uncertain if decay from metastable state included.SEQ given for reaction sequence specifiedUND the reaction is undefined, only the sum of outgoing nucleons is known.(DEF) Compiler is uncertain whether the reaction is defined.

,AG,,AA Adler-Adler symmetry coefficient,AH,,AA Adler-Adler asymmetry coefficient,AKE Average kinetic energy of outgoing particle,AKE/DA,* Avgerage kinetic energy of fission fragment at given angle,ALF Capture-to-fission cross section ratio,AMP Scattering amplitude,AP Most probable mass of fission products,AP,* Most probable mass of fragment specified,ARE Resonance area,COR Angular correlation,COR,*/* Angular correlation between particles specified,COR,*/*/* Angular correlation between particles specified,D Average level spacing,DA Differential cross section with respect to angle,DA,* Differential cross section with respect to angle for particle specified,DA/DA Double differential cross section d2σ/dΩ/dΩ,DA/DA,*/* Double diff. cross section d2σ/dΩ(*1)/dΩ(*2),DA/DA/DE Triple diff.cross section d3σ/dA/dO/dE,DA/DA/DE,*/*/* Triple diff.cross section d3σ/dΩ(*1)/dO(*2)/dE(*3),DA/DE Double diff.cross section d2σ/dΩ/dE,DA/DE,* Double diff.cross section d2σ/dΩ/dE of particle specified,DA/DE/DE,*/*/* Triple diff.cross section d3σ/dΩ(*1)/dE(*2)/dE(*3),DA/KE,* Kinetic energy of fission fragment specified with respect to angle,DA/TYA,P Differential cross section with respect to Treiman-Yang angle,DE Energy spectrum of outgoing particles,DE,* Energy spectrum of particle specified,ECO Energy correlation,EMC Effective mass correlation,EN Resonance energy,ETA Neutron yield (η),ETA/NU η /ν

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,FM/DA Angular distribution, of 1st kind,FM2/DA Spin-polarization probability of 1st kind,INT Cross-section integral over incident energy,J Spin J,KE,* Kinetic energy of fission fragments specified,KER Kerma factor,L Momentum l,LDP Level density parameter,MCO Linear momentum correlation,MLT Multiplicity of outgoing particle,MLT,* Multiplicity of particle specified,NU Total neutron yield (ν),PHS Relative phase,PN Delayed neutron emission probability,POL Spin-polarization probability,POL,* Spin-polarization probability of particle specified,POL/DA Spin-polarization probability dσ/dΩ,POL/DA,* Diff. spin-polarization probability dσ/dΩ of particle specified,PTY Parity,PY Product yield,RAD Scattering radius,RI Resonance integral,SCO Spin-cut-off factor,SGV Reaction rate (s*velocity),SIG Cross section,SIG,* Cross section for production of particle specified,SIG/RAT Cross section ratio,SIG/TMP Temperature-dependent cross section,SPC Gamma spectrum,SPC/DA Gamma spectrum as function of angle,STF Strength function,SWG Statistical weight factor g,TEM Nuclear temperature,TTT Thick-target yield per unit time,TTT/DA Thick-target yield per unit time dY/dΩ,TTY Thick-target yield,TTY/DA Differential thick target yield dY/dΩ,TTY/DA/DE Differential thick target yield dY/dΩ/dE,TTY/DE Differential thick target yield dY/dE,WID Resonance width, Γ,WID/RED Reduced width, Γ0

,ZP Most probable charge of fission products1,WID Resonance width for channel 12,DE Energy spectrum of 2nd secondary particle2,WID Resonance width for channel 23,WID Resonance width for channel 3

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4,WID Resonance width for channel 4BA,AMP Bound-atom scattering amplitudeBA,SIG Bound-atom cross sectionBA/COH,AMP Bound-atom coherent scattering amplitudeBA/PAR,AMP Partial bound-atom scattering amplitudeBIN,AKE,* Average kinetic energy of fission fragment specifiedBIN,AP,* Most prob. mass of fission fragment specified in binary fissionBIN,SIG Binary fission cross sectionBIN/TER,DA/RAT,* Binary/ternary differential dist. dσ/dΩ of fission fragment specifiedBIN/TER,SIG/RAT Binary/ternary cross section ratioCHG,FY Total element yield of fission productsCHG,FY/DE Total element fission yield, differential dY/d(fragment energy)CHN,FY Total chain yield of fission productsCHN,FY/DE Total chain fission yield, differential dY/d(fragment energy)CN,DA Differential cross section dσ/dΩ, compound nucleus contributionCN,FY Fission-product yield, compound nucleus contributionCN,NU ?v, compound nucleus contributionCN,PY Product yield, compound nucleus contributionCN,SIG Cross section, compound nucleus contributionCN/PAR,SIG Partial cross section, compound nucleus contributionCOH,AMP Coherent scattering amplitudeCOH,SIG Coherent cross sectionCUM,FY Cumulative fission-product yieldCUM,FY/RAT Cummulative fission-product yield isomeric ratioCUM/TER,FY Cumulative fission product yield for ternary fissionDI,DA Differential c/s dσ/dΩ, direct interaction contributionDI,DA/DE Double diff. c/s d2σ/dΩ/dE, direct interaction contributionDI,SIG Cross section, direct interaction contributionDI/PAR,DA Partial diff. c/s dσ/dΩ, direct interaction contributionDI/PAR,DA/DE Partial double diff. c/s d2/dA/dE, direct interaction contributionDI/PAR,SIG Partial cross section, direct interaction contributionDL,AKE,* Average kinetic energy of delayed particle specifiedDL,DE,* Delayed energy spectrum of particle specifiedDL,NU Delayed neutron yieldDL,SIG,* Delayed emission cross section of particle specifiedDL,SPC Intensity of delayed gammasDL/PAR,AKE,* Average kinetic energy for specified delayed particle groupDL/PAR,DE,* Energy spectrum for specific delayed particle groupDL/PAR,NU Partial yield of delayed neutronsDL/PAR,SIG,* Partial delayed emission cross section for particle specifiedEM,DA Particle emission angular distributionEM,DA/DE Double differential emission cross section, dσ/dΩ/dEEM,DE Particle emission energy spectrumEM,SIG Emission cross sectionEM/PAR,DA Particle emission partial differential cross section, dσ/dΩEM/PAR,SIG Partial emission cross section

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D.29

EP,DA Partial differential cross section dσ/dΩ for electric polarityEP,SIG Cross section for electric polarityEP/PAR,INT Cross section integral over incident energy for electric polarityEP/PAR,SIG Partial cross section for electric polarityFA,SIG Free-atom cross sectionFA/COH,SIG Free-atom coherent scattering cross sectionFA/INC,SIG Free-atom incoherent scattering cross sectionFA/PAR,AMP Partial free-atom scattering amplitudeHEN,SIG ’High-energy’ component of cross sectionINC,AMP Incoherent scattering amplitudeINC,SIG Incoherent scattering cross sectionIND,FY Independent fission yieldIND,FY,* Independent yield of particle specified from prompt fission prod.IND,FY/DE Differential independent fission yield dY/d(fragment energy)IND,FY/RA Independent fission yield ratioIND/TER,FY Independent fission yield for ternary fissionLEN,SIG ’Low-energy’ component of cross sectionMP,SIG Cross section for magnetic polarity givenPAR,ARE Partial resonance areaPAR,COR Partial reaction, angular correlationPAR,DA Partial differential cross section, dσ/dΩPAR,DA,* Partial differential cross section, dσ/dΩ, of particle specifiedPAR,DA/DA Partial double differential cross section d2σ/dΩ/dΩPAR,DA/DA,*/* Partial double differential cross section d2σ/dΩ(*1)/dΩ(*2)PAR,DA/DA/DE,*/*/* Partial triple differential cross section d3σ/dΩ(*1)/dΩ(*2)/dE(*3)PAR,DA/DE Partial double differential cross section dσ/dΩPAR,FM/DA Partial differential cross section, dσ/dΩ, for polynomial of 1st kindPAR,INT/DA,* Integral over incident en. of partial diff. c/s, dσ/dΩ, of particle specifiedPAR,MLT,* Partial multiplicity of particle specifiedPAR,NU Partial yield of neutrons νPAR,POL/DA Differential spin-polarization probability for partial reactionPAR,SIG Partial cross sectionPAR,SIG,* Partial cross section for particle specifiedPAR,STF Partial strength functionPAR,TTY Partial thick target yieldPAR,TTY,* Partial thick target yield for particle specifiedPAR,WID Partial widthPOT,RAD Potential scattering radiusPOT,SIG Potential scattering cross sectionPR,AKE,N Average kinetic energy of prompt neutronsPR,COR,N/N Angular correlation of prompt neutronsPR,COR/DE,N/FF Angle-energy correlation of prompt neutrons with fission fragmentsPR,DA,N Differential cross section, dσ/dΩ of prompt neutronsPR,DA/DE,N Double differential cross section of prompt neutrons, d2σ/dΩ/dEPR,DE,N Energy spectrum of prompt fission neutronsPR,NU Prompt neutron yield (ν)

EXFOR Basics

D.30

PR,SIG Prompt cross sectionPR,SPC Intensity of prompt gammasPR/PAR,NU Partial prompt neutron yield (ν)PR/TER,DA,N Ang.dist.of prompt neutrons from ternary fissionPR/TER,NU Promptν for ternary fissionPR/TER,NU/DE,A Promptν for ternary fission as a function of alpha energyPR/TER,SPC Prompt gamma spectrum from ternary fissionPRE,AKE,* Average kinetic energy of fragment specifiedPRE,AP,* Most probable mass, pre-neutron-emission, of fragment specifiedPRE,DA,* Differential cross section, dσ/dΩ, of primary fragments specifiedPRE,DA/KE,* Kinetic energy distribribution, dσ/dΩ, of primary fragment specifiedPRE,DE,* Energy spectrum of primary fragments specifiedPRE,FY Primary fission yieldPRE,FY/DE Primary fission yield dY/d(kinetic energy)PRE,KE,* Kinetic energy of primary fragments specifiedPRE/BIN,FY Primary fission yield, binary fissionPRE/TER,FY Primary fission yield, ternary fissionSEC,AKE,FF Average kinetic energy of post-neutron-emission fragmentSEC,AP,* Most probable mass of post-neutron-emission fragment specifiedSEC,FY Post-neutron-emission fission yieldSEC/CHN,FY Pre-delayed-neutron chain yieldSEC/CHN,FY/DE Pre-delayed-neutron chain yield dY/d(kinetic energy)TER,AKE,* Average kinetic energy of particle specified, ternary fissionTER,AP Most probable mass of fragment, ternary fissionTER,AP,* Most prob. mass of ternary fission fragment specifiedTER,COR,*/* Angular correlation of particle *1 & particle *2, ternary fissionTER,DA,* Differential cross section, dσ/dΩ, of particle specified, ternary fissionTER,DA/DE,* Double-differential cross sect. d2σ/dΩ/dE of particle spec., ternary

fissionTER,DA/KE,* Kinetic energy distribution, dEkin/dΩ, of particle specified, ternary

fissionTER,DE,* Energy spectrum of particle specified, ternary fissionTER,FY Fission yield, ternary fissionTER,FY,* Fission yield of fragment specified, ternary fissionTER,SIG Cross section, ternary fissionTER,SIG,* Cross section of particle specified, ternary fissionTER,ZP Most probable charge of fragment, ternary fissionTER/BIN,SIG/RAT Ternary/binary fission cross section ratio

Dictionary 37: Result Codes: used with the keyword RESULT.

CAPTA g Γn Γγ / ΓFRCUM Fractional cumulative yieldFRIND Fractional independent yieldRVAL R-value

EXFOR Basics

E.1

Appendix E

Example of an EXFOR Entry

Attached is an example of a complete entry in the EXFOR format.

EXFOR Basics

E.2

EXFOR Basics

E.3

TRANS X023 20000424 X005500000000ENTRY X0055 20000424 X005500000001SUBENT X0055001 20000424 X005500100001BIB 11 20 X005500100002INSTITUTE (1USAPEN,4RUSKUR) X005500100003REFERENCE (J,PR/C,49,2549,199405) X005500100004

X005500100005X005500100006

AUTHOR (R.W.ZURMUHLE,Z.LIU,D.R.BENTON,S.BARROW,N.WIMER,Y.MIAO,C.LEE,J.T.MURGATROYD,X.LI,V.Z.GOLDBERG,M.S.GOLOVKOV) X005500100007

X005500100008TITLE Observation of 12C cluster transfer by angularcorrelation measurements X005500100009

FACILITY (VDGT,1USAPEN) X005500100010SAMPLE A 30 microg/cm**2 self-supporting 12C target used. X005500100011METHOD (BCINT,SITA) X005500100012

X005500100013(MAGSP) Deuterons were momentum analyzed in a doublefocusing magnetic spectrometer. X005500100014

DETECTOR

(PSSSD) Deuterons were detected in the focal planewith double-sided position sensitive silicondetector covered with a Ta foil to stop beamparticles that otherwise might strike the detector.

X005500100015X005500100016X005500100017X005500100018X005500100019ADD-RES (COMP).Distorted Wave Born Approximation and Hauser

Feshbach Formalism. X005500100020STATUS (APRVD) Approved by author, 5 April 2000. X005500100021HISTORY (20000327C) X005500100022ENDBIB 22 0 X005500100023NOCOMMON 0 0 X005500100024ENDSUBENT 23 0 X005500199999SUBENT X0055002 20000424 X005500200001BIB 6 15 X005500200002REACTION (6-C-12(7-N-14,D+A)10-NE-20,PAR,DA/CRL) X005500200003

(E-EXC1,12-MG-24) X005500200004(E-EXC2,10-NE-20) X005500200005ANG1 is angle between incident beam and deuterons. X005500200006

EN-SEC

ANG2 is angle between deuterons and alpha particles. X005500200007X005500200008X005500200009X005500200010

DETECTOR An annular detector subdivided into ten segments,also used at small angles. Each annulus had a widthof 12 mm and was separated from adjacent segmentswith 1-mm wide inactive masks. X005500200011(DATA-ERR) Uncertainty read from figures. X005500200012ERR-ANALYS(ANG2-ERR) Data-point reader uncertainty. X005500200013(1.) Data taken with the annular detector. X005500200014

X005500200015FLAG

(2.) Data taken with position sensitive stripdetectors. X005500200016

STATUS (CURVE) Data scanned from Fig.3 in reference. X005500200017ENDBIB 15 0 X005500200018COMMON 4 3 X005500200019ANG1 E-EXC1 E-EXC2 ANG2-ERR X005500200020ADEG MEV MEV ADEG X005500200021 0. 13.45 0. 0.4 X005500200022ENDCOMMON 3 0 X005500200023DATA 5 95 X005500200024EN ANG2-CM DATA DATA-ERR FLAG X005500200025MEV ADEG ARB-UNITS ARB-UNITS NO-DIM X005500200026 33. 8.0 71. 16. 1. X005500200027 33. 11.3 34. 8. 1. X005500200028 33. 14.5 35. 7. 1. X005500200029

EXFOR Basics

E.4

33. 16.7 30. 4. 2. X005500200030 33. 17.3 26. 5. 1. X005500200031

... ... ... ... ... 33. 108.0 11.0 4.0 2. X005500200075 42. 11.4 28.0 4. 1. X005500200076 42. 15.9 17.7 2. 1. X005500200077 42. 17.7 18.7 2.5 2. X005500200078 42. 19.9 16.7 1.8 1. X005500200079

... ... ... ... ... 42. 112.7 5.9 1.5 2. X005500200122ENDDATA 97 0 X005500200123ENDSUBENT 122 0 X005500299999SUBENT X0055003 20000424 X005500300001BIB 3 3 X005500300002REACTION (6-C-12(7-N-14,D+A)10-NE-20,PAR,DA,D) X005500300003ERR-ANALYS (DATA-ERR) Relative uncertainty given. X005500300004STATUS Data taken from Table III in reference. X005500300005ENDBIB 3 X005500300006COMMON 1 3 X005500300007EN E-EXC X005500300008MEV MEV X005500300009 33. 13.45 X005500300010ENDCOMMON 3 X005500300011DATA 3 5 X005500300012ANG DATA DATA-ERR X005500300013ADEG MB/SR PER-CENT X005500300014 6.01 0.39 10. X005500300015 12.3 0.40 10. X005500300016 18.3 0.27 11. X005500300017 30.4 0.28 11. X005500300018 36.5 0.27 11. X005500300019ENDDATA 7 X005500300020ENDSUBENT 19 X005500399999SUBENT X0055004 20000424 X005500400001BIB 3 3 X005500400002REACTION (6-C-12(7-N-14,D+A)10-NE-20,PAR,SIG) X005500400003ANALYSIS (INTAD) X005500400004ERR-ANALYS (DATA-ERR) Absolute uncertainty given. X005500400005STATUS (DEP,X0055003) Data taken from text in reference. X005500400006ENDBIB 3 X005500400007NOCOMMON 0 0 X005500400008DATA 3 1 X005500400009EN E-LVL DATA DATA-ERR X005500400010MEV MEV MB MB X005500400011 33. 13.45 3.6 0.5 X005500400012ENDDATA 3 X005500400013ENDSUBENT 12 X005500499999ENDENTRY 3 X005599999999ENDTRANS 1 Z999999999999