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Hypothesis Testing in Noninferiority and Equivalence MRMC ROC Studies

Rationale and Objectives

Conventional multireader multicase receiver operating characteristic (MRMC ROC) methodologies use hypothesis testing to test differences in diagnostic accuracies among several imaging modalities. The general MRMC-ROC analysis framework is designed to show that one modality is statistically different among a set of competing modalities (ie, the superiority setting). In practice, one may wish to show that the diagnostic accuracy of a modality is noninferior or equivalent, in a statistical sense, to that of another modality instead of showing its superiority (a higher bar). The purpose of this article is to investigate the appropriate adjustments to the conventional MRMC ROC hypothesis testing methodology for the design and analysis of noninferiority and equivalence hypothesis tests.

Materials and Methods

We present three methodological adjustments to the updated and unified Obuchowski-Rockette (OR)/Dorfman-Berbaum-Metz (DBM) MRMC ROC method for use in statistical noninferiority/equivalence testing: 1) the appropriate statement of the null and alternative hypotheses; 2) a method for analyzing the experimental data; and 3) a method for sizing MRMC noninferiority/equivalence studies. We provide a clinical example to further illustrate the analysis of and sizing/power calculation for noninferiority MRMC ROC studies and give some insights on the interplay of effect size, noninferiority margin parameter, and sample sizes.

Results

We provide detailed analysis and sizing computation procedures for a noninferiority MRMC ROC study using our method adjusted from the updated and unified OR/DBM MRMC method. Likewise, we show that an equivalence hypothesis test is identical to performing two simultaneous noninferiority tests (ie, either modality is noninferior to the other).

Conclusion

Conventional MRMC ROC methodology developed for superiority studies can and should be adjusted appropriately for the design and analysis of a noninferiority/equivalence hypothesis testing. In addition, the confidence interval of the difference in diagnostic accuracies is important information and should generally accompany the statistical analysis and any conclusions drawn from the hypothesis testing.

Multireader multicase receiver operating characteristic (MRMC ROC) analysis is a popular approach to evaluating and comparing the diagnostic accuracy of medical imaging modalities . A commonly used statistical tool for comparing the diagnostic accuracy of two or more imaging modalities is hypothesis testing. Methods of hypothesis testing in MRMC ROC studies have been investigated extensively, for example, the DBM (Dorfman-Berbaum-Metz) method and the OR (Obuchowski-Rockette) method . These methods have been further updated and compared and, more recently, the DBM and the OR methods are unified for the analysis and power estimation of multireader ROC studies . In these methods, the null and alternative hypotheses are generally defined as follows: under the null hypothesis (denoted as H 0 ), the diagnostic accuracies (eg, areas under the ROC curve, or AUC) of all the modalities are equal; under the alternative hypothesis (denoted as H 1 ), they are not all equal (ie, at least one is significantly different from the others). The goal of the study is to reject the null hypothesis and demonstrate there is a difference or superiority, the success of which can be claimed by obtaining a P value (Type I error rate) that is less than a prespecified significance level α (eg, 0.05).

Although superiority of diagnostic accuracy is often the driving force for scientific innovation, meeting this high bar is not always necessary for accepting a new technology into clinical practice. For example, when a new imaging modality offers lower or equivalent radiation dose to the patient than does the conventional modality and has similar diagnostic accuracy (ie, noninferior performance), it would be appropriate for use in the clinic. Another example could be demonstrating that a computer-aided diagnosis (CAD) system works equally well on images obtained from multiple image acquisition systems where equivalent performance among the various imaging systems would provide evidence of the robustness of the CAD system across different image acquisition systems.

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Materials and methods

Statement of Hypotheses

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Figure 1, Illustration of the null and alternative hypotheses in equivalence and noninferiority tests.

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Table 1

Statements of the Hypotheses in Four Types of Hypothesis Testing Settings

Two-sided One-sided Nonequivalence Superiority H 0 : e − c = 0 H 0 : e − c = 0 H 1 : e − c ≠ 0 H 1 : e − c > 0 Equivalence Noninferiority H 0 : | e − c | = δ H 0 : e − c = −δ H 1 : | e − c | < δ H 1 : e − c > −δ

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Analysis of Data for Noninferiority Tests

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t=ˆe∙−ˆc∙+δsˆ, t

=

e

c

+

δ

s

,

where ˆi∙

i

• is the estimated average reader AUC for modality i ( i = e,c ) and the dot symbol represents an average over readers, sˆ s

is the estimated standard deviation (SD) of ˆe∙−ˆc∙+δ

e

c

+

δ ,

sˆ=2JMS(T∗R)+2H(coˆv2−coˆv3)−−−−−−−−−−−−−−−−−−−−−−−−−−√, s

=

2

J

M

S

(

T

R

)

+

2

H

(

c

o

v

2

c

o

v

3

)

,

where the function H is defined as H(x) = x if x > 0 and 0 otherwise, coˆv2 c

o

v

2 is the estimated covariance in diagnostic accuracies of different readers in the same modality, coˆv3 c

o

v

3 is the estimated covariance in diagnostic accuracies of different readers in different modalities, and MS(T*R) is the two-way ANOVA test-by-reader mean squares in the OR model,

MS(T∗R)=12(J−1)∑Jj=1[(ˆej−ˆcj)−(ˆe∙−ˆc∙)]2. M

S

(

T

R

)

=

1

2

(

J

1

)

j

=

1

J

[

(

e

j

c

j

)

(

e

c

)

]

2

.

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dˆf0={MS(T∗R)+H(J(coˆv2−coˆv3))}2(MS(T∗R))2/(J−1). d

f

0

=

{

M

S

(

T

R

)

+

H

(

J

(

c

o

v

2

c

o

v

3

)

)

}

2

(

M

S

(

T

R

)

)

2

/

(

J

1

)

.

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[ˆe∙−ˆc∙−sˆtα/2,df0,ˆe∙−ˆc∙+sˆtα/2,df0]. [

e

c

s

t

α

/

2

,

d

f

0

,

e

c

+

s

t

α

/

2

,

d

f

0

]

.

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Sizing/Power Calculation for Noninferiority Tests

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λˆ=d+δ2{σˆ2TR+c∗c[σˆ2ϵ−coˆv1+(J−1)H(coˆv2−coˆv3)]}/J√, λ

=

d

+

δ

2

{

σ

T

R

2

+

c

c

[

σ

ϵ

2

c

o

v

1

+

(

J

1

)

H

(

c

o

v

2

c

o

v

3

)

]

}

/

J

,

dˆf1={σˆ2TR+c∗c[σˆ2ϵ−coˆv1+(J−1)H(coˆv2−coˆv3)]}2{σˆ2TR+c∗c[σˆ2ϵ−coˆv1−H(coˆv2−coˆv3)]}2J−1, d

f

1

=

{

σ

T

R

2

+

c

c

[

σ

ϵ

2

c

o

v

1

+

(

J

1

)

H

(

c

o

v

2

c

o

v

3

)

]

}

2

{

σ

T

R

2

+

c

c

[

σ

ϵ

2

c

o

v

1

H

(

c

o

v

2

c

o

v

3

)

]

}

2

J

1

,

where c ∗ is the case sample size in the pilot study, c and J are the case sample size and the reader sample size, respectively, for the planned study, σˆ2∈ σ

2 is the sum of case variability and the within-reader variability, and the test-reader interaction variance is estimated as

σˆ2TR=MS(T∗R)−σˆ2ϵ+coˆv1+H(coˆv2−coˆv3). σ

T

R

2

=

M

S

(

T

R

)

σ

ϵ

2

+

c

o

v

1

+

H

(

c

o

v

2

c

o

v

3

)

.

Figure 2, Illustration of the distributions of the test statistic under the null and alternative hypotheses.

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Power=1−F(tc;df1,λ|H1), Power

=

1

F

(

t

c

;

df

1

,

λ

|

H

1

)

,

where F(t; df 1 , λ|H__1 ) is the distribution function of the test statistic t under the alternative hypothesis H 1 and t c = F −1 (1-α/2;df 0 |H 0 ).

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Equivalence Tests

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Results

Example

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Table 2

Combinations of Number of Cases and Number Readers for 80% Power in Establishing Noninferiority of Spin-echo MRI as Compared to Cine MRI, Based on the Van Dyke et al Data

Noninferiority Margin δ = 0.01 Noninferiority Margin δ = 0.02σˆ2TR=0 σ

T

R

2

=

0 σˆ2TR=0.0001 σ

T

R

2

=

0.0001 σˆ2TR=0 σ

T

R

2

=

0 σˆ2TR=0.0001 σ

T

R

2

=

0.0001 Readers Cases Power Cases Power Cases Power Cases Power 3 559 0.8005 1898 0.8000 388 0.8003 710 0.8002 4 343 0.8004 491 0.8004 238 0.8001 300 0.8002 5 266 0.8014 330 0.8007 185 0.8020 213 0.8005 6 225 0.8004 263 0.8002 157 0.8023 174 0.8011 7 200 0.8002 227 0.8014 139 0.8005 151 0.8002 8 183 0.8001 203 0.8008 128 0.8029 137 0.8022 9 171 0.8008 187 0.8018 119 0.8016 126 0.8008 10 162 0.8017 174 0.8002 113 0.8035 118 0.8002 11 154 0.8003 165 0.8010 107 0.8005 112 0.8004 12 148 0.8002 158 0.8021 103 0.8011 108 0.8033 13 143 0.8001 152 0.8024 100 0.8028 104 0.8033 14 139 0.8005 146 0.8001 97 0.8024 100 0.8008 15 136 0.8021 142 0.8009 94 0.8003 97 0.8001

MRI, magnetic resonance imaging.

The abnormal to normal case ratio in the planned study is assumed to be the same as that in the Van Dyke data (ie, 45/69 = 0.652). The effect size d is 0.04 as measured in the Van Dyke study.

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Discussion

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H0:e−(c−δ)=0 H

0

:

e

(

c

δ

)

=

0

H1:e−(c−δ)>0, H

1

:

e

(

c

δ

)

0

,

and comparing to the superiority test ( Table 1 ), we see immediately that to show e is noninferior to c appears isomorphic with showing e is superior to cδ .

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Acknowledgment

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