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ELEMENTS OF PROBABILTY … A. N. Kolmogorov (1933) + … ) , , ( P B Carlos Mana Carlos Mana Benasque-2014 Benasque-2014 Astrofísica y Física de Partículas Astrofísica y Física de Partículas CIEMAT CIEMAT

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Page 1: ELEMENTS OF PROBABILTY … A. N. Kolmogorov (1933) + … Carlos Mana Benasque-2014 Astrofísica y Física de Partículas CIEMAT

ELEMENTS OF PROBABILTY

… A. N. Kolmogorov (1933) + …

),,( PBCarlos Mana Carlos Mana Benasque-2014Benasque-2014Astrofísica y Física de PartículasAstrofísica y Física de PartículasCIEMATCIEMAT

Page 2: ELEMENTS OF PROBABILTY … A. N. Kolmogorov (1933) + … Carlos Mana Benasque-2014 Astrofísica y Física de Partículas CIEMAT

Event: Object of questions that we make about the result of the experiment suchthat the possible answers are: “it occurs” or “it does not occur”

elementary = those that can not be decomposed in others of lesser entity

Sample Space: {Set of all the possible elementary results of a random experiment}

exclusive: if one happens, no other occursexhaustive: any possible elemental result has to be included in

The elementary events have to be:

sure: get any result contained in

impossible: to get a result that is not contained in

random event: any event that is neither impossible nor sure

k

ke

jkjkee jk ,;0is a partition of

)(1) Sample Space

}{ ke

Page 3: ELEMENTS OF PROBABILTY … A. N. Kolmogorov (1933) + … Carlos Mana Benasque-2014 Astrofísica y Física de Partículas CIEMAT

)dim(

Finitedrawing a die

denumerable throw a coin and stop when we get head

654321 ,,,,, eeeeee

,,,, xxxcxxcxcc

non-denumerable decay time of a particle t

Page 4: ELEMENTS OF PROBABILTY … A. N. Kolmogorov (1933) + … Carlos Mana Benasque-2014 Astrofísica y Física de Partículas CIEMAT

),( B2) Measurable Space

B

Sample Space

-algebra (Boole) Class closed under complementation and denumerable union

We are interested in a class of events that:

1) Contains all possible results of the experiment on which we are interested

2) Is closed under union and complementation

BAABABAA 21121 ;,

BWhy algebra ?

;;;;0; 212121 BAABAABAABB

1) has all the elementary events (to which we shall assign probabilities)2) has all the events we are interested in (deduce their probabilities)B

So now:

Page 5: ELEMENTS OF PROBABILTY … A. N. Kolmogorov (1933) + … Carlos Mana Benasque-2014 Astrofísica y Física de Partículas CIEMAT

654321 ,,,,, eeeeee

Several possible algebras:

A={get an even number}

Ā={get an odd number} AAEB ,,0,

0,min EB

of subsetspossibleallEB ,0,max

n)(dim

k

nSubsets with k elements n

n

k k

n2

0

elements

Minimal:

Maximal:

10

0

n 1:

n

n:0

EXAMPLE:

Interest in evenness:

Page 6: ELEMENTS OF PROBABILTY … A. N. Kolmogorov (1933) + … Carlos Mana Benasque-2014 Astrofísica y Física de Partículas CIEMAT

Generalize the Boole algebra such that and can be performed infinite number of times resulting on events of the same class (closed)

BABA

iiii

11

)dim( denumerable

has structure of σ-algebraB

Remember that: 1) All -algebras are Boole algebras 2) Not all Boole algebras are -algebras

has the structure of Boole algebra )dim( finite B

,...1

BAi

i BABA c

Page 7: ELEMENTS OF PROBABILTY … A. N. Kolmogorov (1933) + … Carlos Mana Benasque-2014 Astrofísica y Física de Partículas CIEMAT

In general, in non-denumerable topological spaces there are subsets that can not be considered as events

We are mainly interested innR

linear set of points

Among its possible subsets are the intervals

points

(degenerated interval) aaa ,

,Rany interval,

denumerable or not, is a subset of R

finite or denumerable of intervals is an interval

finite or denumerable ofintervals is not, in general, an interval

Which are the “elementary” events?

0,,, aaaaaa

)dim( non-denumerable

:R

…but…

Page 8: ELEMENTS OF PROBABILTY … A. N. Kolmogorov (1933) + … Carlos Mana Benasque-2014 Astrofísica y Física de Partículas CIEMAT

Generate a σ-algebra, for instance, from half open intervals on the right

ba,

aaanbabanbababnabannn

,1,,1,,,1,111

Contains all half-open intervals on the right

2) Form the set A by adding their denumerable unions and complements

It has all intervals and points (degenerated intervals)

Its elements are Borel sets (borelians)

3.1) There is at least one σ-algebra containing A (add sets to close under denumerable union and complementation)

1) Initial Set (Ω):

RBQZN ,,Ω: intervals assigns P to intervals

3.2) The intersection of any number of σ-algebras is a σ-algebra There exists a smallest σ-algebra

containing ABorel σ-algebra : Minimum σ-algebra of subsets of generated by R)( RB ba,

],[),,(],,( bababa(May do with as well)

Page 9: ELEMENTS OF PROBABILTY … A. N. Kolmogorov (1933) + … Carlos Mana Benasque-2014 Astrofísica y Física de Partículas CIEMAT

RBA :3.1) Measure Set function

i) -additive

),,( B3) Measure Space

11

)(i

ii

i AA 0;,,1,

21

jiji

ji AAAA

0)(: ABA ii) Non-negative

All Borel Sets of Rn are Lebesgue MeasurableThere are non-denumerable subsets of R with zero Lebesgue measure (Cantor Ternary Set)If axiom of choice (Solovay 1970) not all subsets of R are measurable are not Borel (Ex.: Vitali’s set)

1)( 3.2) Probability Measure

),,( PB►Probability Space

Remember that:

P(notation )

►Measure Space ),,( B

Any bounded measure can be converted in a probability measure

RBA 1,0:(certainty)

(univoque)

For any succession of disjoint of sets of B

),...(1)( AAc

Page 10: ELEMENTS OF PROBABILTY … A. N. Kolmogorov (1933) + … Carlos Mana Benasque-2014 Astrofísica y Física de Partículas CIEMAT

Random variables

Associate to each elemental event of the sample space Ω one, andonly one, real number through a function

(misfortunately called “random variable”)

RwXwwX )(:)(

Results of the experiment notnecessarily numeric,…

Induced Space

(f(w):ΩΔ Borel measurable measurable wrt the σ-algebra associated to Ω)

),(),( II BB X

What is random is the outcome of the experiment before it is done; our knowledge on the result before observation,…

Is neither variable nor random),(),( RII BRBE

)( kXP )),(( baXP

Usually:

),,(),,( III PBPB

or

To keep the structure of the σ-algebra it isnecessary that X(w) be Lebesgue (…Borel)measurable

IBABAX ;)(1

RBABAX ;)(1

Page 11: ELEMENTS OF PROBABILTY … A. N. Kolmogorov (1933) + … Carlos Mana Benasque-2014 Astrofísica y Física de Partículas CIEMAT

654321 ,,,,, eeeeee

A={get an even number}

Ā={get an odd number} AAEB ,,0,

EXAMPLE:

Interest in evenness:

RwXwwX )(:)(

1)()()( 321 eXeXeX

1)()()( 654 eXeXeX

],(1 aX

Ba 01Beeea },,{11 321

Ba 1

1)

1)()()( 531 eXeXeX

1)()()( 642 eXeXeX

Ba 01BAeeea },,{11 442

Ba 1

2)

Page 12: ELEMENTS OF PROBABILTY … A. N. Kolmogorov (1933) + … Carlos Mana Benasque-2014 Astrofísica y Física de Partículas CIEMAT

Types of Random Quantities

Discrete Continuous

finite or denumerable set

),,( QBRwwX :)(

),,( PBR RAccording to the Range of X(w) …

non-denumerable set

R

A dPAXP )()()( 1

n

kAk k

xX1

)()( 1simple function:

ofpartitionfinitenkAk ,,1; ► simple random quantity:

RnkRxkX ,,1;

1

)()(k

Ak kxX 1elementary function:

► elementary random quantity:

ofpartitioncountablekAk ,1;

RkRxkX ,1;

setedenumerablnonRX

)()()()( dQAPxXPkAkk 1

)(X

R

A dPAXP )()()( 1

AA

dwfdP )()(

► absolutely continuous:

(Radon-Nikodym Theorem)

► singular

Page 13: ELEMENTS OF PROBABILTY … A. N. Kolmogorov (1933) + … Carlos Mana Benasque-2014 Astrofísica y Física de Partículas CIEMAT

Radon-Nikodym Theorem (1913;1930)

),( Btwo σ-finite measures over the measurable space ,

AAA

wdwfwdd

dvwdvA )()()()(

If

BA

measurable function over with range in (non-negative)unique

)(wf B ,0

(if same properties as ))(wf)(wg 0)()(| xgxfx

Probability density function:

)(w Lebesgue measure

),,( QBRwwX :)(

AXBR

dxxpAQ)(1

)(

),,( PBR R

BAAAcontinuousabsolutely 00)(:

such that

thenwfif )(

Page 14: ELEMENTS OF PROBABILTY … A. N. Kolmogorov (1933) + … Carlos Mana Benasque-2014 Astrofísica y Física de Partículas CIEMAT

0)( xPRxW

Each set Wk has, at most, k points for otherwise

If , then some

W if the denumerable union of finite sets

i

ik xP 1)(

Wx x

Wx

Set of points of R with finite probabilities

so if it is ∞-denumerable, it is not possible that all the points have the same probability

If X is AC 0)( aXP0])([ a but {X=a} is not an impossible result

Remember that:

1K

KWW partition of kW 1)(21

1 xPxW

21)(31

2 xPxW

kxPkxWK1)(1

1 …

…kW

kWxIf , then

The set of points of R with finite probabilities is denumerable

i

ixP 1)(

W is a denumerable set

Page 15: ELEMENTS OF PROBABILTY … A. N. Kolmogorov (1933) + … Carlos Mana Benasque-2014 Astrofísica y Física de Partículas CIEMAT

DISTRIBUTION FUNCTION

Page 16: ELEMENTS OF PROBABILTY … A. N. Kolmogorov (1933) + … Carlos Mana Benasque-2014 Astrofísica y Física de Partículas CIEMAT

Gen.Def: One-dimensional DF RRxF X :

RxxFxF ;)()(lim

0

1)(lim;0)(lim xFxF xx

)()0( xFxF 1)(;0)( FF

Distribution Function

1) Continuous on the right:

2) Monotonous non-decreasing:

)()( 21 xFxF

3) Limits:

2121, xxandRxxif

Page 17: ELEMENTS OF PROBABILTY … A. N. Kolmogorov (1933) + … Carlos Mana Benasque-2014 Astrofísica y Física de Partículas CIEMAT

The Distribution Function of a Random Quantity has all the information needed to describe the properties of the random process.

wXDistribution Function of a Random Quantity

Def.- DF associated to the Random Quantity is the function

RxxXPxXPxF ;,)()(

X

)(11)( xFxXPxXP )()( xFxXP

Properties

)()(,)( 122121 xFxFxxXPxXxP

RxxXPxXPxF ;,)()(

Page 18: ELEMENTS OF PROBABILTY … A. N. Kolmogorov (1933) + … Carlos Mana Benasque-2014 Astrofísica y Física de Partículas CIEMAT

Properties of the DF (some)DF defined

bx

axxF

1

0)( Rba ,

RxXIf takes values in

Set of points of discontinuity of the DF is finite or denumerable

)()( xFxF )()(/ xFxFRxD)()( xFxF

monótona crecienteQxrDx )( such that )()()( xFxrxF

2121 /, xxDxx )()()()( 2211 xrxFxFxr

associated is different for each xis a one-to-one relation

)(xr

monotonous non-decreasing

2)

1)

3)

QxrDx )(

)()()(lim0

xXPxFxF

has a jump of amplitude

)()(,)( xFxFxxXPxXxP

At each point of discontinuity …

)( xXP )(xF

Page 19: ELEMENTS OF PROBABILTY … A. N. Kolmogorov (1933) + … Carlos Mana Benasque-2014 Astrofísica y Física de Partículas CIEMAT

Distribution Function Probability Measure

For each DF there exists a unique probability measure defined over Borel Sets that assigns the probability to each half-open interval

)()( 12 xFxF Rxx 21,

Reciprocally, to each probability measure defined on the measurable space , corresponds a DF

Random Quantitydiscrete

continuous Distribution Function

),( B

singular or absolutely continuous

Page 20: ELEMENTS OF PROBABILTY … A. N. Kolmogorov (1933) + … Carlos Mana Benasque-2014 Astrofísica y Física de Partículas CIEMAT

Discrete Random Quantity XRwX :)(

RX Range of

),,( QB ),,( PBR R

:)(wX finite or

denumerable set

1k

kp

,..., 21 xxX takes values

with probabilities ,..., 21 pp

kp real, non-negative and

ii pxXP )(

1)(;0)( FF

k

kxk xpxXPxF )()()( ],(1DF:

1) Step-wise and monotonous non-decreasing

2) Constant everywhere but on points of discontinuity where it has a jump

kkkk pxXPxFxF )()()(

Page 21: ELEMENTS OF PROBABILTY … A. N. Kolmogorov (1933) + … Carlos Mana Benasque-2014 Astrofísica y Física de Partículas CIEMAT

EXAMPLE:

1i

ip

kk kXPp2

1)(

,...2,1X

k

kxk xpxXPxF )()()( ],(1

kkkk pxXPxFxF )()()(

1)(;0)( FF

Page 22: ELEMENTS OF PROBABILTY … A. N. Kolmogorov (1933) + … Carlos Mana Benasque-2014 Astrofísica y Física de Partículas CIEMAT

Continuous Random Quantity

)(xF continuous everywhere in R )()( xFxF )()()()( xFxXPxFxF

RwX :)(

RX Range of

),,( QB ),,( PBR R

:)(wX non-denumerable set

AC: Radon-Nikodym A AA

dwwpdd

dPdPAP )()(

Lebesgue measure

)(xp Probability Density Function

2) bounded in every bounded interval of and Riemann integrable on it

3)

Rxxp ;0)(1)

R

1)(

dxxp

x

duupxFxXP )()()(

dx

xdFxp

)()( uniquely a.e.

0

Page 23: ELEMENTS OF PROBABILTY … A. N. Kolmogorov (1933) + … Carlos Mana Benasque-2014 Astrofísica y Física de Partículas CIEMAT

21

11)(

xxp

x

duupxF )()(

)arctan(1

2

1x

EXAMPLE:

Page 24: ELEMENTS OF PROBABILTY … A. N. Kolmogorov (1933) + … Carlos Mana Benasque-2014 Astrofísica y Física de Partículas CIEMAT

EXAMPLE: )1,0(~ CsX

1 3n

nnX

X 2,0]supp[ nX

2

1)2()0( nn XPXP

Example

)()( xXPxF

x

duupxF )()(

Page 25: ELEMENTS OF PROBABILTY … A. N. Kolmogorov (1933) + … Carlos Mana Benasque-2014 Astrofísica y Física de Partículas CIEMAT

General Distribution Function (Lebesgue Decomposition)

1)(|)(

dxxpxp

x

duupxF )()(

C SD N

j

N

k

Dkk

ACjj

N

i

Dii xFaxFbxFaxF

1 11

)()()()(

discretediscrete Abs. continuousAbs. continuous SingularSingular

almost everywhere

)(xF0)( xF

continuous

almost everywhere)()( xFxp

pdf:

(Dirac Delta, Cantor,…)

(Normal, Gamma,…)

(Poisson, Binomial,…)

)( nxXP 1)(

nnxXP

Step Function (simple or elementary) with denumerable number

of jumps

Page 26: ELEMENTS OF PROBABILTY … A. N. Kolmogorov (1933) + … Carlos Mana Benasque-2014 Astrofísica y Física de Partículas CIEMAT

CONDITIONAL PROBABILITY and BAYES THEOREM

Given a probability space

● The information assigned to an event

depends on the information we have

Two consecutive extractions without replacement:

What is the probability to get a red ball in the second extraction?

1) I do not know the outcome of the first : P(r)=1/2

2) It was black: P(r)=2/3

All probabilities are conditional

),,( PBBA

Page 27: ELEMENTS OF PROBABILTY … A. N. Kolmogorov (1933) + … Carlos Mana Benasque-2014 Astrofísica y Física de Partículas CIEMAT

Consider

and two not disjoint sets

BBE

)()()()( BAPBAPEAPAP

BBA, 0BA

A and B A and not B

What is the probability for A to happen

if we know that B has already occured?)( BAP

)()( BAPCBAP )()(1)( BPCBBPCBBP

Probability to happen

)(

),()(

BP

BAPBAP

)(1 BPC

Notation: ),,,()( CBAPCBAP

Conditional Probability

Statistical Independence

),(),( BAPBAP

),,( PB

0)( BP

Page 28: ELEMENTS OF PROBABILTY … A. N. Kolmogorov (1933) + … Carlos Mana Benasque-2014 Astrofísica y Física de Partículas CIEMAT

Statistical Independence

)()( APBAP

)()(: APBAP Correlation

Generalization: ),,,( 21 nAAAP

!n possible arrangements

)(),,(),,(),,,( 311221 nnnn APAAAPAAAPAAAP

A Bdoes not depend on

)()(: APBAP )()( APBAP

That B has already happened does not change the probability of ocurrence of A

)(),,(),,( 3221 nnn APAAAPAAAP ),,(),,( 221 nn AAPAAAP

Page 29: ELEMENTS OF PROBABILTY … A. N. Kolmogorov (1933) + … Carlos Mana Benasque-2014 Astrofísica y Física de Partículas CIEMAT

…should say ”inconditionally” independent

Caution !

BAAAA n ,,, 21 For a finite collection of n events

are independent iff:

)()(),( jiji APAPAAP

)()()(),,( kjikji APAPAPAAAP

)()(),,( mpmp APAPAAP

for each subset AAA mp ,,

kji nkji ,,1,, ji nji ,,1,

)()( APBAP A Bindependent of …

)()(),( CBPCAPCBAP It may happen that depends on through A B C

Conditional dependence

)()(),( BPAPBAP but

Page 30: ELEMENTS OF PROBABILTY … A. N. Kolmogorov (1933) + … Carlos Mana Benasque-2014 Astrofísica y Física de Partículas CIEMAT

Theorem of

Total Probability

)()()()(

11k

n

kk

n

kBAPBAPAPAP

nkBk ,1,

0

jji

i BB j

n

jB

1

Partition of the Sample Space

n

kkk

n

kk BPBAPBAPAP

11

)()|(),()(

n

kkk

n

kk BPBAPBAP

11

)()()(

C

BCPBCAPBAP )(),()(

Theorem of Total Probability with Conditional Probabilities)()|(),|(),(),|(),,( BPBCPCBAPCBPCBAPCBAP

C

CBAPBAP ),,(),(

Page 31: ELEMENTS OF PROBABILTY … A. N. Kolmogorov (1933) + … Carlos Mana Benasque-2014 Astrofísica y Física de Partículas CIEMAT

… to find out a method by which we might judge concerning the probability that an event has to happen, in given circumstances, upon supposition that we know nothing concerning it but that, under the same circumstances, it has happened a certain number of times, and failed a certain other number of times.

Common sense is indeed sufficient to shew us that, form the observation of what has in former instances been the consequence of a certain cause or action, one may make a judgement what is likely to be the consequence of it another time.

…some rule could be found, according to which we ought to estimate the chance that the probability for the happening of an event perfectly unknown, should lie between any two named degrees of probability, antecedently to any experiments made about it; …

Bayes Theorem

LII. An Essay towards solving a Problem in the Doctrine of Chances. By the late Rev. Mr. Bayes, communicated by Mr. Price, in a letter to John Canton, M. A. and F. R. S.

Dear Sir,Read Dec. 23, 1763. I now send you an essay which I have found among the papers of our deceased friend Mr. Bayes, and which, in my opinion, has great merit, and well deserves to be preserved. Experimental philosophy, you will find, is nearly interested in the subject of it; and on this account there seems to be particular reason for thinking that a communication of it to the Royal Society cannot be improper.

The Reverend Thomas Bayes, F.R.S. (1701?-1761)

Page 32: ELEMENTS OF PROBABILTY … A. N. Kolmogorov (1933) + … Carlos Mana Benasque-2014 Astrofísica y Física de Partículas CIEMAT

)()()()(),( APABPBPBAPBAP

)(

)()()(

AP

HPHAPAHP ii

i

nkH k ,1, Partition of the Sample Space

ni ,1

Probability of occurrence of the event (cause, hypothesis) Hi “a priori”, before we know if event A has happened

Probability of occurrence of event A having occurred (cause, hypothesis) Hi

Probability (“a posteriori”) fo event Hi to happen having observed the occurrence of event (efect) A

Probability thatProbability that HHii be the cause (hypothesis) of the observed effect A be the cause (hypothesis) of the observed effect A

normalisation

)(

)()()(

AP

BPBAPABP

Page 33: ELEMENTS OF PROBABILTY … A. N. Kolmogorov (1933) + … Carlos Mana Benasque-2014 Astrofísica y Física de Partículas CIEMAT

n

kkk

iii

HPHAP

HPHAPAHP

1

)()(

)()()(

n

kkk

ii

i

HPHHPHAP

HPHHPHHAPHAHP

100

000

0

)()()(

)()(),(),(

Other forms of

Bayes Theorem:

BT+ Total Probability Theorem

+ general hypothesis (H0) (all probabilities are condicional)

… and many more to come…

n

kkk HPHAPAP

1

)()()(

nkH k ,1, Partition of the Sample Space

),( 0HAP

Page 34: ELEMENTS OF PROBABILTY … A. N. Kolmogorov (1933) + … Carlos Mana Benasque-2014 Astrofísica y Física de Partículas CIEMAT

),(),( 221121 xXxXPxxF

),( 21 xxp

2211 ),()( dxxxpxp

)()|()()|(),( 22111221 xpxxpxpxxpxxp

1212 ),()( dxxxpxp

)(

),()|(

1

2112 xp

xxpxxp

Def

)(

),()|(

2

2121 xp

xxpxxp

Def

)0)(( xp

)()|( 212 xpxxp

)()|( 121 xpxxp

Marginal and Conditional DensitiesMarginal and Conditional Densities

21

221121 ),(),(xx

dwwwpdwxxF

(Stieltjes-Lebesgue integral )

Page 35: ELEMENTS OF PROBABILTY … A. N. Kolmogorov (1933) + … Carlos Mana Benasque-2014 Astrofísica y Física de Partículas CIEMAT

EXAMPLE: CAUSE-EFFECT

is sic:1H

:12 HH is healthy

Hypothesis o causes to analyze

exclusive y exhaustive

Dat

a

incidence in the population

“a priori” probabilities 1000

1)( 1 HP

1000

999)(1)( 12 HPHP

if T denotes the event

T={give positive in the test } 100

99)( 1 HTP

100

2)( 1 HTP

Certain disease occurs in 1 out of 1000 individuals

There is a diagnostic test such that:

If a person is sic, gives positive in the 99% of the cases

If a person is healthy, gives positive in 2% of the cases

A person has given positive in the test. What are the chances that he is sic?

A person has given positive.

What are the chances that he is sic? ???)( 1 THP

Page 36: ELEMENTS OF PROBABILTY … A. N. Kolmogorov (1933) + … Carlos Mana Benasque-2014 Astrofísica y Física de Partículas CIEMAT

)(

)()()( 11

1 TP

HPHTPTHP

2

1

)()()(k

kk HPHTPTP

Bayes Theorem:Bayes Theorem:

Total Probability Theorem:Total Probability Theorem:

047.0

1000999

1002

10001

10099

10001

10099

)()()(

)()()(

1

111

n

kkk HPHTPTP

HPHTPTHP

The test is costly, agresive,… if a person gives positive… The test is costly, agresive,… if a person gives positive…

What are the chances that he is healty?What are the chances that he is healty?953.0)(1)( 11 THPTHP

The disease is serious… The disease is serious…

What are the chances to be sic giving negative in the test?What are the chances to be sic giving negative in the test?

511111 10

)(1

)())(1(

)(1

)()()(

TP

HPHTP

TP

HPHTPTHP

be sicbe sic:1H T={give positive in the test } T={give positive in the test }

99.0)( 1 HTP !!!!

Page 37: ELEMENTS OF PROBABILTY … A. N. Kolmogorov (1933) + … Carlos Mana Benasque-2014 Astrofísica y Física de Partículas CIEMAT

xHP )( 1Incidence of the disease in the population

Probability to be sic giving positive )1()()(

)()(

11

11

xHTPxHTP

xHTPTHP

)1()()(

)1()()(

11

1

1xHTPxHTP

xHTPTHP

Probability to be healthy giving positive

Probability to be sic giving negative

)(1

))(1(

)(1

)()( 11

1 TP

xHTP

TP

xHTPTHP

Probabilities of interest as function of known data and incidence of the disease in the population

)1()()(1

))(1(

11

1

xHTPxHTP

xHTP

Page 38: ELEMENTS OF PROBABILTY … A. N. Kolmogorov (1933) + … Carlos Mana Benasque-2014 Astrofísica y Física de Partículas CIEMAT

x

xTHP

101102)( 1

x

xTHP

972

)1(2)( 1

x

xTHP

972

99)( 1

From the given data:Interest to minimise )( 1 THP )( 1 THP

maximize )( 1 THP

)( 1HPx

optimum

eficiency

healthy giving positive

sic undetected

undergo costly and agresive treatment

correctly detected sic

incidence in the population

Page 39: ELEMENTS OF PROBABILTY … A. N. Kolmogorov (1933) + … Carlos Mana Benasque-2014 Astrofísica y Física de Partículas CIEMAT

),( cHP

),( cHP ),( cHP

),( cHP

HH

Receiver Operating Characteristic

(ROC curve)

)max())(( 22 dxxfd

c

duufcFcHP )()(),( 11

c

duufcFcHP )()(),( 22

))(()()( 1212 xFFxfcFx

1

0

121

1

0

))(()( dxxFFdxxfA

For each cut value c

Tru

e po

siti

ve P

(+|H

)

)1,0( )1,1(

5.0A),( xx

)),(( xxf

optimum

random

u

dxxfduufduufuFA )()()()( 1221

)( HP False positives

)1,0(T

rue

posi

tives

Tru

e po

sitiv

es

)( HP

False PositivesFalse Positives

)( HP

Reverse selection criteria

)0,0(

Page 40: ELEMENTS OF PROBABILTY … A. N. Kolmogorov (1933) + … Carlos Mana Benasque-2014 Astrofísica y Física de Partículas CIEMAT

STOCHASTIC CHARACTERISTICS

Page 41: ELEMENTS OF PROBABILTY … A. N. Kolmogorov (1933) + … Carlos Mana Benasque-2014 Astrofísica y Física de Partículas CIEMAT

n

kAk k

xX1

)()( 1

),,( QBRX :)(

),,( PBR

1

)()(k

Ak kxX 1

R

Akk dPAPxXPk

)()()()( 1

AAR

A dwfdPdPAXP )()()()()( 1

k

kk xXPxg )()(

RR

dxxfxgxdFxg )()()()(

R

dPXgXgEYE )()]([)]([][

Def.: Expectation:Def.: Expectation:

)(X Discrete

)(X Absolutely continuous

)]([ XgY

As usual:

(Stieltjes-Lebesgue integral )

Mathematical ExpectationMathematical Expectation

Page 42: ELEMENTS OF PROBABILTY … A. N. Kolmogorov (1933) + … Carlos Mana Benasque-2014 Astrofísica y Física de Partículas CIEMAT

R

dxxxpXE )(][

R

nnn dxxpxXE )(][

i

ii XccX 0 i

ii XEccXE ][][ 0

i

iXX i

iXEXE ][][

)()( 1 RLxpxn

nmn nmn 02 nif 10

niiX 1}{ independent

MomentsMoments (wrt origin)

Mean:Mean:

Linear operator

Rci ►

R

nn dxxpcxcXE )()(])[(

Rc

])[(min 2cXERc c

Moments Moments wrt point

…Moments wrt Mean

Page 43: ELEMENTS OF PROBABILTY … A. N. Kolmogorov (1933) + … Carlos Mana Benasque-2014 Astrofísica y Física de Partículas CIEMAT

R

dxxpxXEXV )0()()(])[(][ 222 Variance:Variance:

R

nnn dxxpxXE )()(])[(

33

1 3

44

2

221

2][ XY cYV NOT Linear► XccY 10

Skewness: Kurtosis:

Moments wrt MeanMoments wrt Mean

01

11

limlim1

1

n

kk

k

k kka

a

Poisson!

)(k

ekXPk

!)(

00 kkekXPX

k

k

n

k

nn

n

)1(

1)(

2xxp

Cauchy

dxxpxn |)(| 1n

)1( nforCPV

No moments (no mean, no variance,…)

)()( 1 RLxpxn Watch!!Watch!!

Abs. Conv.

22

6)(

nnXP

,2,1n

1];[ kXE kk

,2,1,0k

Page 44: ELEMENTS OF PROBABILTY … A. N. Kolmogorov (1933) + … Carlos Mana Benasque-2014 Astrofísica y Física de Partículas CIEMAT

Right

Dispersion: Variance

Position: Mean: , …

Mode: )(sup0 xpx x Median: 2/1)()( mm xXPxF qxXPxF )()(quantile:

2

0x 0

0

0

344

2

Asymmetry: Skewness 33

1 Symmetric

Left

0

0

0

Peaked: Kurtosis Normal

01 Mode < Median < Mean 01 Mode > Median > Mean

Global PictureGlobal Picture

][XE

mx

Page 45: ELEMENTS OF PROBABILTY … A. N. Kolmogorov (1933) + … Carlos Mana Benasque-2014 Astrofísica y Física de Partículas CIEMAT

2121221121 ][)])([(],[ XXEXXEXXV

},{ 21 XX independent 0],[ 21 XXV

1],[

121

2112

XXV

Covariance Covariance (and “Linear Correlation” )(and “Linear Correlation” )

Linear relation: baXX 12112

212 cXaX Quadratic:

Comments

0,2

1211 thenisXforif

1|| 12 Holder inequality:

Page 46: ELEMENTS OF PROBABILTY … A. N. Kolmogorov (1933) + … Carlos Mana Benasque-2014 Astrofísica y Física de Partículas CIEMAT

)()()(),(),( 222

),(211

),(12121

2121

ijDOxx

gx

x

ggXXgY

)(),()],([][ 22121 ijDOgXXgEYE

)()(][ 22

),(211

),(12121

xx

gx

x

gYEY

][2][][ 21

),(212

2

21

2

121)2,1()2,1(

XXVx

g

x

gXV

x

gXV

x

g

1221

),(21

22

2

2

21

2

121)2,1()2,1(

2

x

g

x

g

x

g

x

g

22][][ YYEYEYV

),,( 21 XXgY Taylor Expansion for the Variance of

(mind for the re-maind-er…)

Useful expression:

iiXE )(

Page 47: ELEMENTS OF PROBABILTY … A. N. Kolmogorov (1933) + … Carlos Mana Benasque-2014 Astrofísica y Física de Partículas CIEMAT

INTEGRAL TRANSFORMS

Fourier (… Laplace) TransformMellin Transform

Page 48: ELEMENTS OF PROBABILTY … A. N. Kolmogorov (1933) + … Carlos Mana Benasque-2014 Astrofísica y Física de Partículas CIEMAT

CRf :

dxxfet ixt )()()(1 RLf Rt

Properties:

Fourier Transform (Characteristic Function)

Probability Density…

][)( ixteEt

1)( t

)()( tt

1)0( ►

► bounded

►Schwarz symmetry

►Uniformly continuous in R

Exists for all

Inversion Theorem (Lévy,1925)

dttexp itx )(2

1)(

dttexXp kitxk )(

2

1)(

b

b

itxk dtte

bxXp k

/

/

)(2

)(

Discrete:

Reticular: bnaxk ZnbRba ,0,,

► One-to-one correspondence between DF and CF► Two DF with same CF are the same a.e.

CRt :

)()(|,0 tt

(all necessary but not sufficient)

)(X

Page 49: ELEMENTS OF PROBABILTY … A. N. Kolmogorov (1933) + … Carlos Mana Benasque-2014 Astrofísica y Física de Partículas CIEMAT

niiii xpX 1)}(~{

nXXX 1

If are n independent random quantities

)()(][)( 1)( 1 tteEt n

XXitX

n

21 XXX )()()()()( 2121 tttttX

][][)()( )( tXigiYtY eEeEtXgY

bXaY Rba ,

)()( btet Xiat

Y

Useful Relations:

If distribution of is symmetric, then is a real function X )(tX

)()()()( tttt XXXX

Page 50: ELEMENTS OF PROBABILTY … A. N. Kolmogorov (1933) + … Carlos Mana Benasque-2014 Astrofísica y Física de Partículas CIEMAT

)|(~ 111 nPoX

)|(~ 222 nPoX21 XXX

)1()(it

i ei et

C

zzw

n

n

dzezi

enXP

S )/1(2)1(

2/

2

1

2)(

Pole of order n+1 at z=0

0

2/21

)1()1(

)(]0),({Re

p

pn

pnpzzfs

)2()( 21)(

2/

2

1 21

n

n

IenXP

)()(21

2121)()()(itit ee

X eettt

X: Discrete reticular: a=0, b=1

],(;:

2/1

2

1

zC

c

Example

Page 51: ELEMENTS OF PROBABILTY … A. N. Kolmogorov (1933) + … Carlos Mana Benasque-2014 Astrofísica y Física de Partículas CIEMAT

)|(~ kkk xPoX

),|(~ kkkk xNX

),|(~ kkkk baxCaX

),|(~ kkk baxGaX

)|(~ SxPoX

),|(~ SSxNX

nXXX 1

nS 1

nS 1

221

2nS

nS aaa 1

nS bbb 1

),|(~ SS baxCaX

),|(~ SbaxGaXnS bbb 1

Some Useful Cases:

Page 52: ELEMENTS OF PROBABILTY … A. N. Kolmogorov (1933) + … Carlos Mana Benasque-2014 Astrofísica y Física de Partículas CIEMAT

)1,0(~ CsX

][)( iXteEt0

)()(][

t

k

kkk t

tiXE

itiXt eeEt 212

1][)(

1 3n

nnX

X

2,0]supp[ nX

2

1][

2)0()1 XE

i

8

1

8

3][

8

3)0( 22)2 XE

2

1)2()0( nn XPXP

Moments of a Distribution (F-LT usually called “moment generating functions)

][),,( )(1

111 ntXtXin eEtt

0,,

1

1

),,()(][

n

j

j

i

ijiji

tt

n

jk

k

ik

kkkk

jki tt

ttiXXE

Example

Page 53: ELEMENTS OF PROBABILTY … A. N. Kolmogorov (1933) + … Carlos Mana Benasque-2014 Astrofísica y Física de Partículas CIEMAT

CRf :

0

1)();( dxxxfsfM s

)(1 RLf

Cs Obviously, if exists …

)()(lim0

xOxfx

)()(lim xOxfx

)Re(s

Strip of holomorphyProbability Densities…

i

i

sdsxsfMi

xf

),(

2

1)(

,

,)Re(

][);( 1 sXEsfM

Mellin Transform

Re

Im

,);( sfM

xexf )(1 1)(2 xexf

)();( 2,1 ssfM ,0 0,1

0 1 0

Page 54: ELEMENTS OF PROBABILTY … A. N. Kolmogorov (1933) + … Carlos Mana Benasque-2014 Astrofísica y Física de Partículas CIEMAT

baXY 0,, aRba

)1()( 1 bbsMasM Xs

Y

1XY1,1 ba )2()( sMsM XY

niiii xpX 1)}(~{

),0[ ix

nXXXX 21independent

Non- negative

121 XXX

)()()( 1 sMsMsM nX

)2()()( 21 sMsMsM X

Useful Relations:

Page 55: ELEMENTS OF PROBABILTY … A. N. Kolmogorov (1933) + … Carlos Mana Benasque-2014 Astrofísica y Física de Partículas CIEMAT

c

)|(~ 222 axExX

)|(~ 111 axExX1

)()(

s

i

ia

ssM21XXX

121

2

)(

)()(

sX aa

ssM

ic

ic

z dzzxaai

aaxp 2

2121 )()(

2)(

,0

0c real

)2(2)( 21021 xaaKaaxp

Newman series…

)ln()1(2)1(

)(]),({Re 212

21 xaann

xaanzzfs

n

n

Example

Page 56: ELEMENTS OF PROBABILTY … A. N. Kolmogorov (1933) + … Carlos Mana Benasque-2014 Astrofísica y Física de Partículas CIEMAT

)|(~ 222 axExX

)|(~ 111 axExX

21XXX

)2(2~ 21021 xaaKaa

121 XXX

21221 )(~ xaaaa

),|(~ 1111 baxGaX

),|(~ 2222 baxGaX)2(

)()(

2~ 21

12/)(2

1

2

21

21 21

21

xaaKxa

a

bb

aav

bbbb

012 bb21

121

)()()(

)(~

21

121

21

21bb

bbb

xaa

xaa

bb

bb

121 a

|)|(~ 021 xaKa

XXX

),0|(~ 111 xNX

),0|(~ 222 xNX

…Densities with support in R…

Some Useful Cases:

0

21 )()()( dwwpxwpxp

0

211)/()()( dwwwxpwpxpobviously…

Page 57: ELEMENTS OF PROBABILTY … A. N. Kolmogorov (1933) + … Carlos Mana Benasque-2014 Astrofísica y Física de Partículas CIEMAT

DISTRIBUTIONS AND GENERALIZED FUNCTIONS

Page 58: ELEMENTS OF PROBABILTY … A. N. Kolmogorov (1933) + … Carlos Mana Benasque-2014 Astrofísica y Física de Partículas CIEMAT

CTDxT ,)(:

DT

cCD `

2121 ,,, TTT

,, TT nn

nn}{

RRf : Locally Lebesgue integrable (LLI) defines a distribution

dxxxfT f )()(,

“regular” distributions (“singular” the rest)

is a Distribution

Linear functional:

Continuous functional:

Distribution Functional:

C ,

Page 59: ELEMENTS OF PROBABILTY … A. N. Kolmogorov (1933) + … Carlos Mana Benasque-2014 Astrofísica y Física de Partículas CIEMAT

,,)(

GTGTae

DGT DGT , C ,

0,0suppsupp TT ,,; TTDD

,, TT ppp DTTD ,)1(,

,,}{ TTiffTT nn

nn

)(,),(, axTaxTTSa

)(,||

1),(, a

xTa

axTTPa

Some Basic Properties (see text for more)

~,,

~TT Fourier Transform

Page 60: ELEMENTS OF PROBABILTY … A. N. Kolmogorov (1933) + … Carlos Mana Benasque-2014 Astrofísica y Física de Partículas CIEMAT

)()(,,, aaxS aa

)0(||

1)(,

||

1,,

aax

aP axa

)(2 ]/1,/1[ xn

f nnn 1

0|)0()0(|lim|,,|lim nnnn

212121 ,,)0()0(, )0(,

)0(,,

,, nnT

)()( ),0[ xxH 1

0

),0[ )()()(, dxxdxxxTH 1

,)0(,, HH

Two examples

LLI: defines a distribution

Page 61: ELEMENTS OF PROBABILTY … A. N. Kolmogorov (1933) + … Carlos Mana Benasque-2014 Astrofísica y Física de Partículas CIEMAT

Tempered Distributions cCD `

“rapidly decreasing” (Schwartz Space)

xexf )( RxRx )()( ),0( xexf x

1

SS

)(1 RLf R

mC

xa

xf

)(

)(2 0Nmfor some

defines a Tempered Distribution fT

)(2 ]/1,/1[ xn

f nnn 1 0|,,| nnT

0C 1C admissible admissible

….

EXAMPLE:

andCCRS |:{ },0||lim 0||

NmnDx nm

x

EXAMPLE:

EXAMPLE:

Sx nn )}({

0,0|)(|max NmkxDx nn

mk

Rx

0)(, nn xT

Convergence to zero

T

Page 62: ELEMENTS OF PROBABILTY … A. N. Kolmogorov (1933) + … Carlos Mana Benasque-2014 Astrofísica y Física de Partículas CIEMAT

),,( QB RX :)(

]),(()()( 1 xXQxXPxF LLI: defines a distribution

,FT

Probability Density “Distribution” ,,, FF TTT

T does not have to be generated by a LLI function

In general In general T is a Probability Distribution if:T is a Probability Distribution if: 00, T

11, T

…but any LLI function defines a probability distribution if

0)(0)()(, xdxxxfT f

1)(1, dxxfT f

,,1)( SDx

Probability Distributions

Page 63: ELEMENTS OF PROBABILTY … A. N. Kolmogorov (1933) + … Carlos Mana Benasque-2014 Astrofísica y Física de Partículas CIEMAT

0

)(!

)(n

nn itn

t

0

)(2

1

!)(

2

1)(

n

nitxnitx dtiten

dttexp

0

) )0,(!

)1(n

nnnp x

nT dtex itx

2

1)0,(

dxxpet itx )()(

delta distribution

0

)

0

) )0(!

),0,(!

)1(,n

nn

n

nnnp n

xn

T

pDPROB TTT )1(

)(X ,,)( 21 xxXrec )( kk xXPp

1

)(k

kkD xpT

RXrec )( )()( xxp RA1

Delta Distribution unifies discrete and AC random quantities:

Discrete:

Continuous:

CF:

Page 64: ELEMENTS OF PROBABILTY … A. N. Kolmogorov (1933) + … Carlos Mana Benasque-2014 Astrofísica y Física de Partículas CIEMAT

)()()()()()()()()( 221 bxHxFbxHaxHaFaxHxHxFxF

)()()()()()()()0()0( ),[2),0[1121 xxfxxfaaFaFFDf ba 11

´,,, FF TDfT

b

ma

mmm

mm dxxxfdxxxfaaFaFFXDfXE )()()()()0(, 2

0

11201

b

a

dxxfdxxfaFaFF )()()()()0(1 2

0

1121

Example

)(1 aF

)(2 aF

)0(1F

1

)(1 xF

)(2 xF

ba0

Page 65: ELEMENTS OF PROBABILTY … A. N. Kolmogorov (1933) + … Carlos Mana Benasque-2014 Astrofísica y Física de Partículas CIEMAT

LIMIT THEOREMS and

CONVERGENCE

Page 66: ELEMENTS OF PROBABILTY … A. N. Kolmogorov (1933) + … Carlos Mana Benasque-2014 Astrofísica y Física de Partículas CIEMAT

Find the limit behaviour of a sequence of random quantities

convergence criteria

General Problem:

,...,...,, 21 nXXX

,...1

,...,2

,1

21211

n

kkn X

nZ

XXZXZ

Example:

How is distributed when ?nZ )( n

~“distance”

1) More or less strong,2) May have convergence for some criteria and not for others

Page 67: ELEMENTS OF PROBABILTY … A. N. Kolmogorov (1933) + … Carlos Mana Benasque-2014 Astrofísica y Física de Partículas CIEMAT

Convergence in:

Distribution

Probability

Norm)(RLp

Almost Sure

Uniform

Central Limit Theorem

Weak Law of Large Numbers

Strong Law of Lage Numbers

Glivenko-Cantelli Theorem

Convergence in Quadratic Mean

Glivenko-Cantelli Theorem

Logarithmic

Page 68: ELEMENTS OF PROBABILTY … A. N. Kolmogorov (1933) + … Carlos Mana Benasque-2014 Astrofísica y Física de Partículas CIEMAT

Chebyshev Theorem

X 2, with finite mean and variance

2

1

kkXP

k

XgEkXgP

)]([)(

)(~ xFX 0)( XgY

?kYP

kXgX )(1 kXgX )(2 21 X

21

)()()()(][ xdFxgxdFxgYE

0

0)( Xg

2

))(()( 2 kXgkPXkPxkdF

kXg )(

2)()( XXg

Bienaymé-Chebyshev Inequality

Page 69: ELEMENTS OF PROBABILTY … A. N. Kolmogorov (1933) + … Carlos Mana Benasque-2014 Astrofísica y Física de Partículas CIEMAT

Let be r.q. with the same distribution and finite mean

,...,...,, 21 nXXX ),...(),...,(),( 2211 nn xFxFxF

nX X if, and only if

0;0)(lim XxXP nn

o, equivalently,

converges in probability to

Convergence in Probability

Let

Def.:

0;1)(lim XxXP nn

and

,...,...,, 21 nXXX Weak Law of Large Numbers (J. Bernouilli…)

0;0lim nn ZP

lim(Prob)

,...1

,...,2

,1

21211

n

kkn X

nZ

XXZXZThe sequence converges in Probability to

LLN in practice:…

WLLN: When n is very large, the probability that Zn differs from μ by a small amount is very small

Zn gets more and more concentrated around the real number μ

But “very small “ is not zero: it may happen that for some k>n, Zk differs from μ by more than ε…

Page 70: ELEMENTS OF PROBABILTY … A. N. Kolmogorov (1933) + … Carlos Mana Benasque-2014 Astrofísica y Física de Partículas CIEMAT

,...,...,, 21 nXXX

nX X if, and only if

0;0)(lim XxXP nn

o, equivalently,

converges “almost sure” to

Convergence Almost Sure Let

Def.:

0;1)(lim XxXP nn

Strong Law of Large Numbers (E.Borel, A.N. Kolmogorov,…)

0;0)(lim xZP nn

Prob(lim)

Let be r.q. with the same distribution and finite mean ,...,...,, 21 nXXX

,...1

,...,2

,1

21211

n

kkn X

nZ

XXZXZThe sequence converges Amost Sure to

LLN in practice:…

WLLN: When n is very large, the probability that Zn differs from μ by a small amount is very small

Zn gets more and more concentrated around the real number μ

But “very small “ is not zero: it may happen that for some k>n, Zk differs from μ by more than ε…SLLN: as n grows, the probability for this to happen tends to zero

Page 71: ELEMENTS OF PROBABILTY … A. N. Kolmogorov (1933) + … Carlos Mana Benasque-2014 Astrofísica y Física de Partículas CIEMAT

,...,...,, 21 nXXX ),...(),...,(),( 2211 nn xFxFxF

nX )(~ xFX if, and only if

)(;)()(lim)()(lim FCxxXPxXPxFxF nnnn

o, equivalently,

tends to be distributed as

Rtxxnn ;)()(lim

Convergence in DistributionLet

Def.:

and their corresponding

,...,...,, 21 nXXX

,...1

,...,2

,1

21211

n

kkn X

nZ

XXZXZ

Sequence of independent r.q.

How is distributed when ?nZ )( n

same distribution

2,finite mean and variance

Form the sequence

nzNX

nZ

n

kkn

,~1

1

1,0~~

zN

n

ZZ n

n

Central Limit Theorem (Lindberg-Levy,…)

easy dem. from CF

standarized

Page 72: ELEMENTS OF PROBABILTY … A. N. Kolmogorov (1933) + … Carlos Mana Benasque-2014 Astrofísica y Física de Partículas CIEMAT

n

kkn X

nZ

1

1 1n 2n

5n 10n

20n 50n

Unifom DF

Page 73: ELEMENTS OF PROBABILTY … A. N. Kolmogorov (1933) + … Carlos Mana Benasque-2014 Astrofísica y Física de Partículas CIEMAT

Parabolic DF

n

kkn X

nZ

1

1

1n 2n

5n 10n

20n 50n

Page 74: ELEMENTS OF PROBABILTY … A. N. Kolmogorov (1933) + … Carlos Mana Benasque-2014 Astrofísica y Física de Partículas CIEMAT

Cauchy DF

n

kkn X

nZ

1

1

1n 2n

5n 10n

20n 50n

Page 75: ELEMENTS OF PROBABILTY … A. N. Kolmogorov (1933) + … Carlos Mana Benasque-2014 Astrofísica y Física de Partículas CIEMAT

,...,...,, 21 nxxx

Glivenko-Cantelli Theorem

If observations are iid: 10)()(suplimlim xFxFP nxnn

The Empiric Distribution Function converges uniformly to the Distribution Function of the r.q. X

)(ne

)1(e one observation of X }{ 1x

n

kkxn xI

nxF

1],( )(

1)(

number of values xi lower or equal to x

n

Empiric Distribution Function

)(xF

Uniform Convergence

(example of aplication of Chebishev Th.)

)(xf

0)()(suplim

xfxfnSxxn

converges uniformly to 1)( nn xfThe sequence if, and only ifDef.:

experiment

independent, identically distributed

RSffn :,

Page 76: ELEMENTS OF PROBABILTY … A. N. Kolmogorov (1933) + … Carlos Mana Benasque-2014 Astrofísica y Física de Partículas CIEMAT

],( 0xA )(xIY A is a Bernouilli random quantity )()()1( 0xFAXPYP

)(1)()0( 0xFAXPYP )(1)()( 00 xFxFet it

Y

n

knkxn xnFxIZ

1],( )()(

)(xnFZW nn knk FFk

nkWP

)1()(

nFWE

)1( FnFWV

2

)1()()(

n

FFxFxFP n

Demonstration of Convergence in Probability:

n

kkxn xI

nxF

1],( )(

1)(Empiric Distribution Function

with Characteristic Function

1)

2) Sum of iid Bernouilli random quantities

2

1

kkXP

3) Bienaymé-Chebyshev Inequality

is a Binomial r.q.

FFE n

n

FFFV n

)1(

n

WxFn )(

Page 77: ELEMENTS OF PROBABILTY … A. N. Kolmogorov (1933) + … Carlos Mana Benasque-2014 Astrofísica y Física de Partículas CIEMAT

Convergence in Lp(R) Norm

1)( nn wX )(wX

if, and only if,

Converges in norm to Def.:

p=2 convergence in quadratic mean

)(RLp

nRLwX pn ;)()( andRLwX p )()( 0)()(lim p

nn wXwXE

p

n wXwXEnnn )()()(|)(0 00that is:

Logarithmic Divergence of a pdf Xp xx ;)(~

from its true pdf )(xp

Kullback-Leibler “Discrepancy” (see Lect. on Information)

xx

xx d

p

ppppD

X

KL )(~)(

log)(]|~[

1)( iip xA sequence of pdf “Converges Logarithmically” to a density iff)(xp

0]|[lim kKLk ppD

Logarithmic Convergence