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Detection Theory Composite tests Detection Theory

Detection Theory - Lunds tekniska högskola...Detection Theory Chapter 6: GLRT – Large data records Large in this case does not mean that we use Szegö and the Fourier transform

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Page 1: Detection Theory - Lunds tekniska högskola...Detection Theory Chapter 6: GLRT – Large data records Large in this case does not mean that we use Szegö and the Fourier transform

Detection Theory Composite tests

Detection Theory

Page 2: Detection Theory - Lunds tekniska högskola...Detection Theory Chapter 6: GLRT – Large data records Large in this case does not mean that we use Szegö and the Fourier transform

Chapter 5: Correction

Detection Theory

Thu

I claimed that the above, which is the most general case, was captured by the below

Thu

Page 3: Detection Theory - Lunds tekniska högskola...Detection Theory Chapter 6: GLRT – Large data records Large in this case does not mean that we use Szegö and the Fourier transform

Chapter 5: Correction

Thu

I claimed that the above, which is the most general case, was captured by the below

Thu Thu

Argument was

Page 4: Detection Theory - Lunds tekniska högskola...Detection Theory Chapter 6: GLRT – Large data records Large in this case does not mean that we use Szegö and the Fourier transform

Chapter 5: Correction

Thu

I claimed that the above, which is the most general case, was captured by the below

Thu Thu

Slides have been corrected

This is not correct, since it is limited to the case that C2-C1 is positive semi-definite

Page 5: Detection Theory - Lunds tekniska högskola...Detection Theory Chapter 6: GLRT – Large data records Large in this case does not mean that we use Szegö and the Fourier transform

Chapter 6: UMP - Uniformly most powerful tests

Detection Theory

Thu

Consider the case when the value of A is unknown, but assume A>0

Page 6: Detection Theory - Lunds tekniska högskola...Detection Theory Chapter 6: GLRT – Large data records Large in this case does not mean that we use Szegö and the Fourier transform

Chapter 6: UMP - Uniformly most powerful tests

Detection Theory

Thu

Consider the case when the value of A is unknown, but assume A>0

Thu UMP: An optimal test no matter the value of A – similar concept to MVU

Page 7: Detection Theory - Lunds tekniska högskola...Detection Theory Chapter 6: GLRT – Large data records Large in this case does not mean that we use Szegö and the Fourier transform

Chapter 6: UMP - Uniformly most powerful tests

Detection Theory

Thu

Consider the case when the value of A is unknown, but assume A>0

Thu UMP: An optimal test no matter the value of A – similar concept to MVU

Strategy to get UMPs: 1. Design test as if A is known 2. Show that test does not need knowledge of the value A

Page 8: Detection Theory - Lunds tekniska högskola...Detection Theory Chapter 6: GLRT – Large data records Large in this case does not mean that we use Szegö and the Fourier transform

Chapter 6: UMP - Uniformly most powerful tests

Detection Theory

Thu

Step 1: Design test as if A is known

Page 9: Detection Theory - Lunds tekniska högskola...Detection Theory Chapter 6: GLRT – Large data records Large in this case does not mean that we use Szegö and the Fourier transform

Chapter 6: UMP - Uniformly most powerful tests

Detection Theory

Step 1: Design test as if A is known

Page 10: Detection Theory - Lunds tekniska högskola...Detection Theory Chapter 6: GLRT – Large data records Large in this case does not mean that we use Szegö and the Fourier transform

Chapter 6: UMP - Uniformly most powerful tests

Detection Theory

Step 1: Design test as if A is known

Cancel multiplicative constants Remove ”exp” by taking logarithm Cancel x2[n]

Page 11: Detection Theory - Lunds tekniska högskola...Detection Theory Chapter 6: GLRT – Large data records Large in this case does not mean that we use Szegö and the Fourier transform

Chapter 6: UMP - Uniformly most powerful tests

Detection Theory

Step 1: Design test as if A is known

Manipulate a bit….

Page 12: Detection Theory - Lunds tekniska högskola...Detection Theory Chapter 6: GLRT – Large data records Large in this case does not mean that we use Szegö and the Fourier transform

Chapter 6: UMP - Uniformly most powerful tests

Detection Theory

Step 1: Design test as if A is known

scale

Page 13: Detection Theory - Lunds tekniska högskola...Detection Theory Chapter 6: GLRT – Large data records Large in this case does not mean that we use Szegö and the Fourier transform

Chapter 6: UMP - Uniformly most powerful tests

Detection Theory

Step 1: Design test as if A is known

Test statistic is not dependent on A Threshold seems to be, but is not

Page 14: Detection Theory - Lunds tekniska högskola...Detection Theory Chapter 6: GLRT – Large data records Large in this case does not mean that we use Szegö and the Fourier transform

Chapter 6: UMP - Uniformly most powerful tests

Detection Theory

Step 2: Show that test does not need knowledge of the value A

Page 15: Detection Theory - Lunds tekniska högskola...Detection Theory Chapter 6: GLRT – Large data records Large in this case does not mean that we use Szegö and the Fourier transform

Chapter 6: UMP - Uniformly most powerful tests

Detection Theory

Step 2: Show that test does not need knowledge of the value A

Page 16: Detection Theory - Lunds tekniska högskola...Detection Theory Chapter 6: GLRT – Large data records Large in this case does not mean that we use Szegö and the Fourier transform

Chapter 6: UMP - Uniformly most powerful tests

Detection Theory

Step 2: Show that test does not need knowledge of the value A

Page 17: Detection Theory - Lunds tekniska högskola...Detection Theory Chapter 6: GLRT – Large data records Large in this case does not mean that we use Szegö and the Fourier transform

Chapter 6: UMP - Uniformly most powerful tests

Detection Theory

Threshold does not depend on PFA

Step 2: Show that test does not need knowledge of the value A

Page 18: Detection Theory - Lunds tekniska högskola...Detection Theory Chapter 6: GLRT – Large data records Large in this case does not mean that we use Szegö and the Fourier transform

Chapter 6: UMP - Uniformly most powerful tests

Detection Theory

Compute PD

Page 19: Detection Theory - Lunds tekniska högskola...Detection Theory Chapter 6: GLRT – Large data records Large in this case does not mean that we use Szegö and the Fourier transform

Chapter 6: UMP - Uniformly most powerful tests

Detection Theory

Compute PD

Page 20: Detection Theory - Lunds tekniska högskola...Detection Theory Chapter 6: GLRT – Large data records Large in this case does not mean that we use Szegö and the Fourier transform

Chapter 6: UMP - Uniformly most powerful tests

Detection Theory

Compute PD

Page 21: Detection Theory - Lunds tekniska högskola...Detection Theory Chapter 6: GLRT – Large data records Large in this case does not mean that we use Szegö and the Fourier transform

Chapter 6: UMP - Uniformly most powerful tests

Detection Theory

Compute PD

Performance depends on A

Page 22: Detection Theory - Lunds tekniska högskola...Detection Theory Chapter 6: GLRT – Large data records Large in this case does not mean that we use Szegö and the Fourier transform

Chapter 6: UMP - Uniformly most powerful tests

Detection Theory

Recap

A test is UMP if it, for all possible values of the unknown parameter(s), maximzes PD for given PFA

Page 23: Detection Theory - Lunds tekniska högskola...Detection Theory Chapter 6: GLRT – Large data records Large in this case does not mean that we use Szegö and the Fourier transform

Chapter 6: One-sided vs. Two sided

Detection Theory

Consider now: A<0

Page 24: Detection Theory - Lunds tekniska högskola...Detection Theory Chapter 6: GLRT – Large data records Large in this case does not mean that we use Szegö and the Fourier transform

Chapter 6: One-sided vs. Two sided

Detection Theory

Consider now: A<0

Step 1: Design test as if A is known

Same steps as before

Page 25: Detection Theory - Lunds tekniska högskola...Detection Theory Chapter 6: GLRT – Large data records Large in this case does not mean that we use Szegö and the Fourier transform

Chapter 6: One-sided vs. Two sided

Detection Theory

Consider now: A<0

Step 1: Design test as if A is known

Same steps as before

Next thing was to divide with A This changes inequality with A<0

Page 26: Detection Theory - Lunds tekniska högskola...Detection Theory Chapter 6: GLRT – Large data records Large in this case does not mean that we use Szegö and the Fourier transform

Chapter 6: One-sided vs. Two sided

Detection Theory

Consider now: A<0

Step 1: Design test as if A is known

Same steps as before

Next thing was to divide with A This changes inequality with A<0 <

Page 27: Detection Theory - Lunds tekniska högskola...Detection Theory Chapter 6: GLRT – Large data records Large in this case does not mean that we use Szegö and the Fourier transform

Chapter 6: One-sided vs. Two sided

Detection Theory

Consider now: A<0

<

Page 28: Detection Theory - Lunds tekniska högskola...Detection Theory Chapter 6: GLRT – Large data records Large in this case does not mean that we use Szegö and the Fourier transform

Chapter 6: One-sided vs. Two sided

Detection Theory

Consider now: A<0

<

Page 29: Detection Theory - Lunds tekniska högskola...Detection Theory Chapter 6: GLRT – Large data records Large in this case does not mean that we use Szegö and the Fourier transform

Chapter 6: One-sided vs. Two sided

Detection Theory

Consider now: A<0

<

Page 30: Detection Theory - Lunds tekniska högskola...Detection Theory Chapter 6: GLRT – Large data records Large in this case does not mean that we use Szegö and the Fourier transform

Chapter 6: One-sided vs. Two sided

Detection Theory

Consider now: A<0

<

Page 31: Detection Theory - Lunds tekniska högskola...Detection Theory Chapter 6: GLRT – Large data records Large in this case does not mean that we use Szegö and the Fourier transform

Chapter 6: One-sided vs. Two sided

Detection Theory

Consider now: A<0

Page 32: Detection Theory - Lunds tekniska högskola...Detection Theory Chapter 6: GLRT – Large data records Large in this case does not mean that we use Szegö and the Fourier transform

Chapter 6: One-sided vs. Two sided

Detection Theory

This means problems, since test can not be implemented

For A>0, decide H1 if For A<0, decide H1 if

Page 33: Detection Theory - Lunds tekniska högskola...Detection Theory Chapter 6: GLRT – Large data records Large in this case does not mean that we use Szegö and the Fourier transform

Chapter 6: One-sided vs. Two sided

Detection Theory

This means problems, since test can not be implemented

For A>0, decide H1 if For A<0, decide H1 if

UMP exists (one sided)

UMP does not exist (two sided)

Page 34: Detection Theory - Lunds tekniska högskola...Detection Theory Chapter 6: GLRT – Large data records Large in this case does not mean that we use Szegö and the Fourier transform

Chapter 6: One-sided vs. Two sided

Detection Theory

This means problems, since test can not be implemented

For A>0, decide H1 if For A<0, decide H1 if

UMP exists (one sided)

UMP does not exist (two sided)

An educated guess would be to decide H1 if This will turn out to be well motivated by the GLRT that comes shortly

Page 35: Detection Theory - Lunds tekniska högskola...Detection Theory Chapter 6: GLRT – Large data records Large in this case does not mean that we use Szegö and the Fourier transform

Chapter 6: Karlin-Rubin Thm - A condition for UMP

Detection Theory

If the likelihood ratio is monotonic in the test T(x)

and it is known that then Detect H1, if T(x) > γ is UMP

Page 36: Detection Theory - Lunds tekniska högskola...Detection Theory Chapter 6: GLRT – Large data records Large in this case does not mean that we use Szegö and the Fourier transform

Detection Theory

If the likelihood ratio is monotonic in the test T(x)

and it is known that then Detect H1, if T(x) > γ is UMP

This follows directly from the Neyman-Pearson theorem

Chapter 6: Karlin-Rubin Thm - A condition for UMP

Page 37: Detection Theory - Lunds tekniska högskola...Detection Theory Chapter 6: GLRT – Large data records Large in this case does not mean that we use Szegö and the Fourier transform

Detection Theory

Application: Exponential family

Chapter 6: Karlin-Rubin Thm - A condition for UMP

Page 38: Detection Theory - Lunds tekniska högskola...Detection Theory Chapter 6: GLRT – Large data records Large in this case does not mean that we use Szegö and the Fourier transform

Detection Theory

Application: Exponential family

Likelihood ratio

Chapter 6: Karlin-Rubin Thm - A condition for UMP

0

Page 39: Detection Theory - Lunds tekniska högskola...Detection Theory Chapter 6: GLRT – Large data records Large in this case does not mean that we use Szegö and the Fourier transform

Detection Theory

Application: Exponential family

Likelihood ratio: If p(θ) is increasing, then LLR is monotonic in

Chapter 6: Karlin-Rubin Thm - A condition for UMP

0

Page 40: Detection Theory - Lunds tekniska högskola...Detection Theory Chapter 6: GLRT – Large data records Large in this case does not mean that we use Szegö and the Fourier transform

Detection Theory

Application: Exponential family

Likelihood ratio: If p(θ) is increasing, then LLR is monotonic in

In our case (DC level), we have p(θ) = θ/σ2

Chapter 6: Karlin-Rubin Thm - A condition for UMP

0

Page 41: Detection Theory - Lunds tekniska högskola...Detection Theory Chapter 6: GLRT – Large data records Large in this case does not mean that we use Szegö and the Fourier transform

Chapter 6: Composite tesiting – Bayesian approach

Detection Theory

With likelihoods containing unknown parameters,

We can integrate away the unknown

Page 42: Detection Theory - Lunds tekniska högskola...Detection Theory Chapter 6: GLRT – Large data records Large in this case does not mean that we use Szegö and the Fourier transform

Chapter 6: Composite tesiting – Bayesian approach

Detection Theory

With likelihoods containing unknown parameters,

We can integrate away the unknown

A case that is very common and fully doable is x=Hθ+w, with Gaussian matrix H

Page 43: Detection Theory - Lunds tekniska högskola...Detection Theory Chapter 6: GLRT – Large data records Large in this case does not mean that we use Szegö and the Fourier transform

Chapter 6: Composite tesiting – Bayesian approach

Detection Theory

With likelihoods containing unknown parameters,

We can integrate away the unknown

If prior is unknown, use a non-informative one (See Estimation theory book)

Page 44: Detection Theory - Lunds tekniska högskola...Detection Theory Chapter 6: GLRT – Large data records Large in this case does not mean that we use Szegö and the Fourier transform

Detection Theory

Chapter 6: GLRT – Finite data records

The Generalized Likelihood ratio test is heuristic for finite data records, but can be proven optimal asymptotically in the size of the data record

𝐴 = 𝜋𝑟2

Where 𝜽 1 is the MLE of θ under H1, 𝜽 0 is the MLE of θ under H0

Page 45: Detection Theory - Lunds tekniska högskola...Detection Theory Chapter 6: GLRT – Large data records Large in this case does not mean that we use Szegö and the Fourier transform

Detection Theory

Chapter 6: GLRT – Finite data records

Example: Non-coherent detection

𝐴 = 𝜋𝑟2

Page 46: Detection Theory - Lunds tekniska högskola...Detection Theory Chapter 6: GLRT – Large data records Large in this case does not mean that we use Szegö and the Fourier transform

Detection Theory

Chapter 6: GLRT – Finite data records

Example: Non-coherent detection

𝐴 = 𝜋𝑟2

GLRT replaces H with its ML estimate

Page 47: Detection Theory - Lunds tekniska högskola...Detection Theory Chapter 6: GLRT – Large data records Large in this case does not mean that we use Szegö and the Fourier transform

Detection Theory

Chapter 6: GLRT – Finite data records

Example: Non-coherent detection

𝐴 = 𝜋𝑟2

Page 48: Detection Theory - Lunds tekniska högskola...Detection Theory Chapter 6: GLRT – Large data records Large in this case does not mean that we use Szegö and the Fourier transform

Detection Theory

Chapter 6: GLRT – Finite data records

Example: Non-coherent detection

𝐴 = 𝜋𝑟2

Page 49: Detection Theory - Lunds tekniska högskola...Detection Theory Chapter 6: GLRT – Large data records Large in this case does not mean that we use Szegö and the Fourier transform

𝐴 = 𝜋𝑟2

Detection Theory

Chapter 6: GLRT – Finite data records

Example:

𝐴 = 𝜋𝑟2 GRLT is

Page 50: Detection Theory - Lunds tekniska högskola...Detection Theory Chapter 6: GLRT – Large data records Large in this case does not mean that we use Szegö and the Fourier transform

𝐴 = 𝜋𝑟2

Detection Theory

Chapter 6: GLRT – Finite data records

Example:

𝐴 = 𝜋𝑟2 GRLT is

But from estimation theory, we have that the MLE of A is

Page 51: Detection Theory - Lunds tekniska högskola...Detection Theory Chapter 6: GLRT – Large data records Large in this case does not mean that we use Szegö and the Fourier transform

𝐴 = 𝜋𝑟2

Detection Theory

Chapter 6: GLRT – Finite data records

Example:

𝐴 = 𝜋𝑟2 GRLT is

But from estimation theory, we have that the MLE of A is

Thus

Page 52: Detection Theory - Lunds tekniska högskola...Detection Theory Chapter 6: GLRT – Large data records Large in this case does not mean that we use Szegö and the Fourier transform

Detection Theory

Chapter 6: GLRT – Finite data records

Example:

Taking logs, and simplification gives

Page 53: Detection Theory - Lunds tekniska högskola...Detection Theory Chapter 6: GLRT – Large data records Large in this case does not mean that we use Szegö and the Fourier transform

Detection Theory

Chapter 6: GLRT – Finite data records

Example:

Taking logs, and simplification gives

Page 54: Detection Theory - Lunds tekniska högskola...Detection Theory Chapter 6: GLRT – Large data records Large in this case does not mean that we use Szegö and the Fourier transform

Detection Theory

Chapter 6: GLRT – Finite data records

Example:

Taking logs, and simplification gives

Thus,

Page 55: Detection Theory - Lunds tekniska högskola...Detection Theory Chapter 6: GLRT – Large data records Large in this case does not mean that we use Szegö and the Fourier transform

Detection Theory

Chapter 6: GLRT – Large data records

Large in this case does not mean that we use Szegö and the Fourier transform.

In this case, we consider large N, but with independent measurements

Two assumptions: 1. Signal is weak

2. MLE attains asymptotic form

Page 56: Detection Theory - Lunds tekniska högskola...Detection Theory Chapter 6: GLRT – Large data records Large in this case does not mean that we use Szegö and the Fourier transform

Detection Theory

Chapter 6: GLRT – Large data records

Large in this case does not mean that we use Szegö and the Fourier transform.

In this case, we consider large N, but with independent measurements

Two assumptions: 1. Signal is weak Means that A is not enormous. Reasonable, otherwise problem is simple

2. MLE attains asymptotic form

Page 57: Detection Theory - Lunds tekniska högskola...Detection Theory Chapter 6: GLRT – Large data records Large in this case does not mean that we use Szegö and the Fourier transform

Detection Theory

Chapter 6: GLRT – Large data records

Large in this case does not mean that we use Szegö and the Fourier transform.

In this case, we consider large N, but with independent measurements

Two assumptions: 1. Signal is weak Means that A is not enormous. Reasonable, otherwise problem is simple

2. MLE attains asymptotic form From Estimation theory

Page 58: Detection Theory - Lunds tekniska högskola...Detection Theory Chapter 6: GLRT – Large data records Large in this case does not mean that we use Szegö and the Fourier transform

Detection Theory

Chapter 6: GLRT – Large data records

Theorem

Setup

Parameter vector to be detected

Differ for H0 and H1

Equal for H0 and H1 (e.g. noise variance)

Page 59: Detection Theory - Lunds tekniska högskola...Detection Theory Chapter 6: GLRT – Large data records Large in this case does not mean that we use Szegö and the Fourier transform

Detection Theory

Chapter 6: GLRT – Large data records

Theorem

Setup

Parameter vector to be detected

Differ for H0 and H1

Equal for H0 and H1 (e.g. noise variance)

Hypotheses to test for

Page 60: Detection Theory - Lunds tekniska högskola...Detection Theory Chapter 6: GLRT – Large data records Large in this case does not mean that we use Szegö and the Fourier transform

Detection Theory

Chapter 6: GLRT – Large data records

Theorem

Setup

Parameter vector to be detected

Differ for H0 and H1

Equal for H0 and H1 (e.g. noise variance)

Hypotheses to test for

Definition of GLRT Note that MLEs of θs differ under H0 and H1

Page 61: Detection Theory - Lunds tekniska högskola...Detection Theory Chapter 6: GLRT – Large data records Large in this case does not mean that we use Szegö and the Fourier transform

Detection Theory

Chapter 6: GLRT – Large data records

Theorem

Statement

𝐴 = 𝜋𝑟2

Page 62: Detection Theory - Lunds tekniska högskola...Detection Theory Chapter 6: GLRT – Large data records Large in this case does not mean that we use Szegö and the Fourier transform

Detection Theory

Chapter 6: GLRT – Large data records

Theorem

Statement

𝐴 = 𝜋𝑟2

Chi-2 variable, r DoF

Page 63: Detection Theory - Lunds tekniska högskola...Detection Theory Chapter 6: GLRT – Large data records Large in this case does not mean that we use Szegö and the Fourier transform

Detection Theory

Chapter 6: GLRT – Large data records

Theorem

Statement

𝐴 = 𝜋𝑟2

Non-central Chi-2 variable, r DoF

Chi-2 variable, r DoF

Page 64: Detection Theory - Lunds tekniska högskola...Detection Theory Chapter 6: GLRT – Large data records Large in this case does not mean that we use Szegö and the Fourier transform

Detection Theory

Chapter 6: GLRT – Large data records

Theorem

Statement

𝐴 = 𝜋𝑟2

Non-central Chi-2 variable, r DoF

Chi-2 variable, r DoF

True value of θr under H1

Page 65: Detection Theory - Lunds tekniska högskola...Detection Theory Chapter 6: GLRT – Large data records Large in this case does not mean that we use Szegö and the Fourier transform

Detection Theory

Chapter 6: GLRT – Large data records

Theorem

Statement

𝐴 = 𝜋𝑟2

Non-central Chi-2 variable, r DoF

Chi-2 variable, r DoF

True value of θr under H1

True value of θs under H1 / H0

Page 66: Detection Theory - Lunds tekniska högskola...Detection Theory Chapter 6: GLRT – Large data records Large in this case does not mean that we use Szegö and the Fourier transform

Detection Theory

Chapter 6: GLRT – Large data records

Theorem

Statement

𝐴 = 𝜋𝑟2

Non-central Chi-2 variable, r DoF

Chi-2 variable, r DoF

True value of θr under H1

True value of θs under H1 / H0

Fisher Inform, Doesn’t depend on H1 or H0

Page 67: Detection Theory - Lunds tekniska högskola...Detection Theory Chapter 6: GLRT – Large data records Large in this case does not mean that we use Szegö and the Fourier transform

Detection Theory

Chapter 6: GLRT – Large data records

Theorem

Statement

𝐴 = 𝜋𝑟2

Non-central Chi-2 variable, r DoF

Chi-2 variable, r DoF

True value of θr under H1

True value of θs under H1 / H0

Fisher Inform, Doesn’t depend on H1 or H0

Fisher information matrix: one does not need to think about H0 or H1. Think like this: Given x, what is the Fisher info for θr ,θs

Page 68: Detection Theory - Lunds tekniska högskola...Detection Theory Chapter 6: GLRT – Large data records Large in this case does not mean that we use Szegö and the Fourier transform

Detection Theory

Chapter 6: GLRT – Large data records

Theorem

Statement

𝐴 = 𝜋𝑟2

Cancels with no nusiance parameters

Page 69: Detection Theory - Lunds tekniska högskola...Detection Theory Chapter 6: GLRT – Large data records Large in this case does not mean that we use Szegö and the Fourier transform

Detection Theory

Chapter 6: GLRT – Large data records

Theorem

Statement

𝐴 = 𝜋𝑟2

Cancels with no nusiance parameters

Since Fisher is pos. def., λ is degraded by nuisance

Page 70: Detection Theory - Lunds tekniska högskola...Detection Theory Chapter 6: GLRT – Large data records Large in this case does not mean that we use Szegö and the Fourier transform

Detection Theory

Chapter 6: GLRT – Large data records

Theorem

Statement

𝐴 = 𝜋𝑟2

Cancels with no nusiance parameters

Since Fisher is pos. def., λ is degraded by nuisance

Larger λ separates the pdfs more, Thus better PD with larger λ

Page 71: Detection Theory - Lunds tekniska högskola...Detection Theory Chapter 6: GLRT – Large data records Large in this case does not mean that we use Szegö and the Fourier transform

Detection Theory

Chapter 6: GLRT – Large data records

Theorem

Statement

𝐴 = 𝜋𝑟2

Cancels with no nusiance parameters

Since Fisher is pos. def., λ is degraded by nuisance

Larger λ separates the pdfs more, Thus better PD with larger λ

So, not surprisingly, nuisance degrades our detection capability

Page 72: Detection Theory - Lunds tekniska högskola...Detection Theory Chapter 6: GLRT – Large data records Large in this case does not mean that we use Szegö and the Fourier transform

Detection Theory

Chapter 6: GLRT – Large data records

Theorem

Statement

𝐴 = 𝜋𝑟2

No nuisance

Note: The test is still difficult, since it is still given by and we need to find the MLEs