EXPERIMENTATION WITH BISMUTH SALTS SOLUTIONS

AND NEW IDEAS FOR CMNS EXPLANATION

D.S. Baranov, O.D. Baranova

Protvino Moscow region, Russiabaranovd@rambler.ru

Objectives

• Goal this job was the investigation of anomalous nuclear processes in the Bi salt experiment after strong electric field impact

• To explain results are attempt used the nuclear molecule model

•  References• 1. D.S. Baranov, O.D. Baranova OBSERVATION

OF THE ISOMERS 212m1Bi AT THE EXPERIMENTS • WITH SOME BISMUTH SALTS AQUEOUS

SOLUTIONS International Conference Isomers in Nuclear and Interdisciplinary Research (INIR-2011)

• 2. . Baranov D.S., Baranova O.D. Production of Neutron-rich Bi Isotopes by Electric Fields. INTERNATIONAL SYMPOSIUM ON EXOTIC NUCLEI (EXON2009). AIP CONFERENCE PROCEEDINGS VOLUME 1224 P 241-246 http://proceedings.aip.org/proceedings

Sample preparation

Experimental set up

Counts in detector №1

0 30 60 90 120 150 180 2100

5

10

15

20

25

30

35

40

45co

un

ts

time (mins)

exp fity0 2 ±0A1 53.17731 ±7.13849t1 59.01378 ±11.09016

nitrate bismuth alpha activity

0 30 60 90 120 150 180 210

0

5

10

15

20

25

30

35

40

Ядро Периодыполураспада

Брен.%

Схемы распадов МэВ

γ-излучение(МэВ)

Деф.м,е кэВ

207Bi 38 лет Э. З. β+ 0,57(98), 1,77 -20058208Bi 3,68·10 5 лет Э. З. 2,614 -18879209Bi 2·1019 лет 100 → α (4,88 ) 205Pb -18268210Bi 5,013 сут ~100 β (1,16 )210Po→α (5,35 ) 206Pb 0,803(0,0011) -14738210Bim1 3·106 лет 99,6 → α (5 ) 206Tl 0,34, 0,61… 271,3e

211Bi 2,14 мин 99,7 → α (6,62) 207Tl 0,351(14) -11865212Bi 60,6мин;2,98·10-6с 64

36 β (2,25 )212Po →α (8,78) 208Pb → α (6,05) 208Tl

0,727(7), 1,62(1,8)…

-8135

212Bim1

25 мин; 2,98·10-6с 33 67

β (2,25)212Po→ α (8,78 ) 208Pb → α (6,05 ) 208Tl

250e

212Bim2 7 мин; 45,1 с 100 β(1,95)212Pom→α(11,68 )208Pb 2200e

213Bi 45,6мин; 4,2·10-6с 97,8 β (1,39) 213Po α (8,38) 209Pb 0,437 -5247214Bi 19,9мин;1,64·10-4с ~100 β (3,26) 214Po α (7,69) 210Pb 0,6(47)… -1209215Bi 7,7мин;1,78·10-3с ~100 β () 215Po → α (7,38 ) 211Pb 1710215Bim1 36,4мин;1,78·10-3с ~100 β () 215Po → α (7,38 ) 211Pb 1347e

216Bi 3,6мин; 0,15с ~100 β () 216Po → α (6,78 ) 212Pb 5970c217Bi 98.5 c; < 10с ~100 β () 217Po → α (6,55 ) 213Pb218Bi 33 с; 3,05 мин ~100 β (5.06 ) 218Po →α (6,0) 214Pb

Scheme of 212Bi decay

Event example

Detector 1 Experiment data 05.10.2007

Photo 18.10.2007 M= 7 : 1 Photo 05.05.2009 Alpha count 10.3+-0.6 Alpha count 17.2+-1.1

Bi isotopes production for 7.5 hours in a closed Si detecto 4 on pieces of bismuth nitrate, made by

the cumulative emissions

dN/dE for alpha

after 70 mins count in the first 70 mins

Alpha to beta time delay

0,0 0,2 0,4 0,6 0,8 1,0 1,2 1,4 1,60

10

20

30

40

Model: ExpDec1 Chi^2 = 0.15816R^2 = 0.98811 y0 0 ±0A1 46.82147 ±9.95447t1 0.36571 ±0.06108

cou

nts

time delay (mcsec)

beta + alpha delayd events

0 2 4 6 8 10 12 14 16 18 20

0

10

20

30

40

dN/dE for electrons

0,0 0,5 1,0 1,5 2,0 2,50

4

8

12

16

20

24

experiment data theor. data /7/

cou

nts

electron energy (MeV)

0,0 0,5 1,0 1,5 2,0 2,5

0

4

8

12

16

20

24

• We detected 210Bi, 212Bi, 212m1Bi, 214Bi.

• Bismuth 211 and 213 were not found.

• Such scheme of decay is impossible for free nucleus. Thus we need to introduce the system of nucleare

Nuclear molecules Atom Vigier

size 100 Fermi

Traces on Si detector surfaceline – Nuclear molecule position

Silicium plate edge near the woll

Crater

Микроскоп фирмы АМФОРА 80*80 мкм

Energy deposition 0.0001 G

Дет.2

Craters

Project:BaranovOwner: INCA OperatorElevation= 35.0 deg. Tilt= 0.0 deg. Azimuth= 0.0 deg.Sample: 19-05-2011Type: DefaultSample is polished and coated with Carbon - thickness (nm): 15.0, density (g/cm3): 2.25.Thresholding has been selected : All quantitative results below 0 sigma have been set to zero.Site: Sample-1 Spectrum: Spectrum 1 19-май-2011 02:05 PMEnergy Resn. Area TOT.AR. L./R.time(s) P.time U(kV) Perr. .0 49.15 273789 83154 70.00/89.41 6 20.00 95.45%Counted by INCAINCA Proc.Option: Oxygen by stoichiometryElmt A.C.% IntC. Wt% 2*Swt% At% Comp% dComp% FormulaS K 6.57 1.0763 6.10 0.50 15.81 15.24 1.25 SO3 5.46Bi M 34.51 0.9324 37.01 2.18 14.71 41.26 2.43 Bi2O3 5.08O 13.38 0.96 69.48 24.00Total 56.50+/- 2.43 CompSum 56.50+/- 2.73 CatSum 10.54 An.Sum 24.00

Site: Sample-2Spectrum: Spectrum 1 19-май-2011 02:38 PMEnergy Resn. Area TOT.AR. L./R.time(s) P.time U(kV) Perr. .0 49.15 273789 111140 100.00/126.33 6 20.00 95.45%Peak omited: 0.800 keVCounted by INCA/Oxygen by stoichiometryINCA Proc.Option: All elements analyzedElmt A.C.% IntC. Wt% 2*Swt% At% Comp% dComp% FormulaN K 5.24 1.2944 4.05 1.96 19.89 15.62 7.56 N2O5 7.14O K 10.06 0.6471 15.54 1.30 66.84 -0.66 < 7.85 O 24.00Bi M 37.10 0.9201 40.32 1.52 13.27 44.95 1.69 Bi2O3 4.76Total 59.91+/- 2.80 CompSum 60.57+/- 7.74 CatSum 11.91 An.Sum 24.00

11C 40.48O 5.63Si 52.80K 0.35

Au 0.74

12C 37.38O 4.32Si 57.13K 0.29

Au 0.87

13C 91.28O 1.20Si 6.91K 0.25Ca 0.12Au 0.24

14C 58.66O 26.87Si 13.62Na 0.34Ca 0.28Au 0.23

15

Si 100.00

16C 17.43O 2.72Si 78.61

Au 1.24

10C 16.91

Si 81.62

Au 1.46

11C 48.91O 3.69Si 39.18N 7.62Au 0.60

12C 37.02O 2.42Si 59.72

Au 0.84

13C 33.85O 3.79Si 60.76K 0.65Au 0.95

14C 20.97O 9.01Si 67.16K 1.67Au 1.20

“Snake” traces

2C 49.63O 31.54Si 5.85Al 2.85 Zn 5.91Bi 4.22

3C 42.44O 9.27Si 45.88Ca 0.13Zn 0.74Br 0.21Au 0.71Bi 0.64

4C 62.19O 14.94Si 18.89Al 0.59 Zn 1.89Au 0.47Bi 1.03

5C 20.44Si 78.26Au 1.30

6C 28.14Si 70.76Au 1.10

7C 51.55O 20.41Al 0.78Si 23.30Zn 2.29Au 0.58Bi 1.09

8C 55.66O 28.16Al 1.63Si 6.03Ca 0.23Cu 0.43Zn 4.86Bi 3.01

9C 58.40O 28.07Al 1.21Si 1.40Zn 4.17Bi 6.74

Tail

Head10C 47.75O 39.67Al 2.03Si 0.44Zn 4.66Cu 0.77Bi 4.67

9C 55.53O 20.97Al 0.80Si 18.04Zn 2.06Au 0.61Bi 1.99

8C 63.79O 12.59Al 0.24Si 21.62Zn 0.77Au 0.49Bi 0.50

1.We have evidens that giant long-lived nuclear molecules were detected in the experiments with bismuth salts solution.

2. We suppous that nuclear molecules are the part of every CMNS prosess.

3. We need to continue our investigations

Conclusion

Thank you

1 Russan CF Conf.

1993 г. Moscow-Blaсk See train