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Topic 2 Nuclear Counting Statistics

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Title: Topic 2 Nuclear Counting Statistics


1
Topic 2 Nuclear Counting Statistics
  • Random vs Systemic Errors
  • Nuclear Counting Statistics
  • Propagation of Errors
  • Application of Statistical Analysis
  • Statistical Analysis

2
Random vs Systemic Errors
  • Types of measurement errors Blunders, Systemic
    and Random Errors
  • Blunders are gross errors such as incorrect
    instrument setting and wrong injection of
    radiopharmaceuticals.
  • Systemic errors are results differing
    consistently from the correct one such as the
    length measurement by warped ruler.
  • Random errors are variations in results from one
    measurement to another (physical limitation or
    variation of the quantity) such as the rate of
    the radiation emission.

3
Accuracy and Precision
  • Measurement results having systemic errors are
    said to be inaccurate
  • Measurements that are very reproducible (same
    result for repeated measurements) is said to be
    precise.
  • It is possible that result is precise but
    inaccurate and vice versa

4
Nuclear Counting Statistics
  • The Poisson Distribution
  • Standard Deviation
  • The Gaussian Distribution

5
Poisson Distribution
  • Defined only for non-negative integer values
  • The probability of getting a certain result N
    when the true value is m P(Nm)e-mmN/N!
  • Variance, ?2, is defined as such that 68.3 of
    the measurement results fall within ? ? of the
    true value m.
  • For Poisson distribution, ?2 m.

6
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7
Nuclear Medicine Counting
  • Nuclear Medicine radionuclide decay counting
    follows Poisson distribution.
  • Nuclear Medicine question is that how good is the
    result N from a single measurement?
  • The assumption is that N?m so that there is 68.3
    chance that m is within the range N??N. ??N is
    uncertainty in N.
  • Percentage uncertainty is defined as V (?N/N) x
    100.

8
Confidence Intervals
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10
Standard Deviation
  • Standard deviation is calculated from the series
    of measurements where the number of measurements,
    n, and the mean value, are known

11
Standard Deviation, Variance and Nuclear Counting
  • Standard Deviation, SD, is an estimation of
    Variance ?.
  • In nuclear counting, SD??N

12
Gaussian Distribution
  • Gaussian distribution is also called Normal
    Distribution.
  • The Equation describe Gaussian distribution is

13
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14
Gaussian Distribution (continued)
  • For large value m, Poisson distribution can be
    approximated by Gaussian distribution
  • Gaussian distribution is defined for any value of
    x (positive integer for Poisson)
  • Variance ?2 can have any value (mean value m for
    Poisson).
  • If there is additional random errors in nuclear
    counting apart from the radionuclide decay, the
    results are described by Gaussian distribution
    with variance, ?2m(?N)2

15
Propagation of Errors
  • Sums and Differences ?(N1?N2?N3?)?N1N2N3
  • Constant Multiplier ?(kN)k?Nk?N and
    percentage uncertainty
    V(kN) ?(kN)/kNx100100 /?N
  • Products and Radios
    V(N1??N2??N3??)
    ?1/N11/N21/N3

16
Exercises 1
  • Given a formula in nuclear medicine
    Yk(N1-N2)/(N3-N4) Show
    that ?YVY?Y/100
    where
    VY is
    the percentage uncertainty of Y

17
Applications of Statistical Analysis
  • Effects of averaging
  • Counting rates
  • Significance of difference between counting
    measurements
  • Effects of background
  • Minimum detectable activity (MDA)
  • Comparing counting systems
  • Estimating required counting times
  • Optimal division of counting times
  • Statistics of ratemeters.

18
Effects of Averaging
  • If n counting measurements are used to compute an
    average result, then, the uncertainty in
    average is

19
Counting Rates
  • If N counts are recorded during time t, then the
    counting rate is RN/t. The uncertainty in
    counting rate is then given by

20
Significance of Difference Between Counting
Measurements
  • Suppose two measurements, N1 and N2. The
    difference ?N1-N2 could be true difference
    between these two counts or just random variation
    of one.
  • If ?lt2?? is considered marginal (5 chance within
    random error)
  • ?gt3?? is considered significant (1 chance) and
    2?? lt?lt3?? is questionable.

21
Effects of Background Counting
22
Effects of Background (continued)
23
Effects of Background (continued)
24
Minimum Detectable Activity
25
Comparing Counting Systems
26
Estimating Required Counting Times
27
Optimal Division of Counting Times
28
Statistical Tests
  • The Chi-Square Test
  • The t-Test
  • The Treatment of Outliers
  • Linear Regression.

29
The Chi-Square Test
  • The ?2 (chi-square) test is used to test whether
    random variations in a set of measurements are in
    fact consistent with Poisson distribution.
  • The formula for calculating ?2 is

30
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31
The chi-square test (continued)
  • The calculated ?2 value is then compared with the
    table (degree of freedom dfn-1)
  • P is the probability that the observed variation
    in a series of n measurements from a Poisson
    distribution would equal or exceed the calculated
    ?2
  • 0.02ltPlt0.98 are acceptable with P0.5 a perfect.
    Plt0.01 the variation is too large and Pgt0.99 is
    too good to be true. 0.01ltPlt0.02 and 0.98ltPlt0.99
    are suspicious.

32
The t-test
  • T-test is used to test the significance of the
    difference between the means from two sets of
    data that whether they are in fact from the same
    Guassian distribution.
  • Different formulas are used for independent and
    paired data sets
  • Independent data are obtained from two different
    groups whilst paired data have some kind of
    correlation between the two measurements.

33
T-test (continued)
  • The formula for the independent data sets is
    (with mean values X1 and X2, standard deviation
    SD1 andSD2, nn1n2-2 and dfn)

34
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35
T-test (continued)
  • The formula for the paired data set is (with
    the difference average, Standard deviation of the
    pair differences SD, number of paired
    measurements n and dfn-1)

36
T-test (continued)
  • The calculated t (from independent and paired
    data) is then compared with the table.
  • The probability of the data sets are in fact from
    the same Gaussian distribution is less than the
    tabled probability if the calculated t is larger
    than the tabled value. Less than 5 is considered
    to be different.

37
Treatment of Outliers
  • The following formula is used for the
    determination of whether or not a data value X is
    an outlier

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39
Treatment of Outliers (continued)
  • If the calculated T is less than the tabled
    value, the probability of the data value to be an
    outlier is less than the tabled probability.
  • Rejection of data must be done with caution.

40
Linear Regression
  • If we suspect that a parameter X is correlated
    with a measured quantity Y such as YabX

41
Linear Regression (continued)
  • we can use the following formula to determine a,b

42
Linear Regression (continued)
  • And carry out statistical analysis (r?1, strong
    correlation)

43
Linear Regression (continued)
  • A preferred test is t-test using the following
    formula (with number of X,Y pair, n and degree of
    freedom, dfn-2)
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