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Fine Structure of the Auditory M100 in Schizophrenia

and Schizoaffective Disorder

Peter Teale, Martin Reite, Donald C. Rojas, Jeanelle Sheeder, and David Arciniegas

Background:

Several studies have demonstrated

anoma-lous asymmetry of the 100-msec latency auditory-evoked

field (M100) in schizophrenia. Recent evidence suggests

this may be a compound component, however. Our study

examines the localization of two M100 subcomponents in

patients with schizophrenia and schizoaffective disorder.

Methods:

Magnetoencephalographic recordings of

audi-tory-evoked fields were obtained for 14 subjects with

schizophrenia, 12 with schizoaffective disorder, and 23

control subjects. Two M100 subcomponents were

identi-fied and localized in each hemisphere.

Results:

Both patient groups exhibited different

lateral-ization compared with control subjects, with the second

subcomponent tending to be less lateralized.

Conclusions:

The second subcomponent may be the major

contributor to previously reported laterality differences.

Future studies might benefit by separating M100

subcom-ponents so that specific functions could be addressed.

Biol Psychiatry 2000;48:1109 –1112 ©

2000 Society of

Biological Psychiatry

Key Words:

Schizophrenia, schizoaffective disorder,

magnetoencephalography, M100, auditory-evoked fields,

laterality

Introduction

P

sychosis has been associated with anomalous brain

asymmetry (Crow 1990). Several studies have

de-scribed abnormal asymmetry of the 100-msec latency

auditory-evoked field component (M100) in schizophrenia

(less asymmetric or more variable in schizophrenia) as a

manifestation of this anomaly (Hajek et al 1997; Reite et

al 1989, 1997; Tiihonen et al 1998). Some evidence

suggests such anomalies in M100 lateralization may be a

manifestation of a different auditory cortical organization

in schizophrenia (Rojas et al 1997). All previous

magne-toencephalography (MEG) studies in schizophrenia,

how-ever, have considered the M100 a unitary component. The

associated evoked potential, designated N100, is generally

considered to be a superposition of responses produced by

as many as six separate sources (Na¨a¨ta¨nen and Picton

1987) having different spatial and temporal characteristics.

Several of these generators are thought to be radial in

orientation and therefore will not produce measurable

magnetic fields. Recent MEG work suggests the M100 is

a compound component (Lu et al 1992; Sams et al 1993;

Teale et al 1998; Zouridakis et al 1998). In normal

subjects, the M100 component may actually be generated

by two active regions separated in time (by 25 msec) and

in space (later source about 0.1 cm anterior in the L

hemisphere, and 0.8 cm anterior in the right hemisphere;

Teale et al 1998).

Independent localization of these two components has

not been reported in subjects with psychosis. In light of the

laterality differences reported in the literature for the

combined component in subjects with psychosis, we

wished to determine if one of the two putative

subcompo-nents might be selectively contributing to the variance

reported for M100 lateralization.

Methods and Materials

Our subject population consisted of 14 individuals with schizo-phrenia (mean age 36.7 6 6 years), 12 with schizoaffective

disorder (mean age 36.8 6 10 year), and 23 control subjects

(mean age 34610 year) recruited from the Denver metropolitan

area. All patients were in outpatient treatment, and most were medicated. All were men. Diagnosis was determined using the Structured Clinical Interview for DSM-IV and review of medical records. Mean age of onset for the subjects with schizophrenia was 21.62 6 5.35 years and 22.00 6 8.24 years for the

schizoaffective group. All were right handed based on the Annett criteria (Annett 1985). All had normal hearing thresholds at 1 kHz as determined by audiometry. Informed consent was ob-tained from all subjects in accordance with the Colorado Multi-ple Institutional Review Board.

Recordings were obtained inside a magnetically shielded room, with subjects semi-reclining in a nonmagnetic chair, using a BTI Model 607 seven-channel second order biomagnetometer with 18-mm coil diameter and 4-cm baseline. A custom bite plate was fabricated for each subject. Sufficient measurements

cen-From Biomagnetic Imaging Laboratory, Department of Psychiatry, University of Colorado Health Sciences Center, and Denver VA Medical Center, Denver, Colorado.

Address reprint requests to Martin L. Reite, M.D., University of Colorado Health Sciences Center, 4200 East Ninth Avenue, Box C268-68, Denver CO 80262. Received January 14, 2000; revised May 17, 2000; accepted May 23, 2000.

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tered over the temporal lobe were made using five instrument positions (53 7 5 35 B-field measurements) on each

hemi-sphere to assure adequate modeling of both generators with a single equivalent current dipole (ECD) at their respective laten-cies. Subjects viewed a silent video throughout the duration of the recording to maintain a reasonably constant attentional state. Stimuli were computer-generated, 30-msec duration (5-msec rise and fall), 85-dB sound pressure level (measured at the ear), 1-kHz tone pips delivered via polyurethane tubing to the ear opposite the hemisphere being recorded. The interstimulus inter-val was fixed at 6 sec.

A sonic digitizer was used to establish a head frame coordinate system and coregister the position of instrument. The X axis was determined by the line connecting the preauricular points (posi-tive X is outward through the right ear). The Y axis was the line orthogonal to the midpoint of the X axis (the origin) and contained in the plane established by the X axis and the nasion (positive Y anterior). The Z axis was normal to X and Y at the midpoint and exits the top of the head (positive Z is above the origin).

Magnetoencephalographic recordings were wide band (0.1–1 kHz) and digitized at a rate of 2.275 kHz. Recordings included a 200-msec prestimulus baseline and 250 msec following stimulus delivery. Artifact-free responses to 50 stimuli were averaged and then filtered with a phase invariant digital filter (24 dB/octave slope) with a pass band of 0 to 55 Hz.

Source localization analysis was performed across the entire poststimulus window from 0 to 245 msec using a single moving ECD in a conductive sphere model (Sarvas 1987) and a sliding 10-msec width time window at 1 msec increments for each hemisphere. The mean B-field amplitude for each coil for the 10-msec window (starting 5 msec before and ending 5 msec after, each time point) was computed by averaging the samples (23) in this interval. To identify the two candidate sources, a goodness of fit measure (F) was computed at each time point by dividing the root mean square (RMS) value of the error (i.e., the difference between the measured field amplitudes and the final iteration of the forward solution) by the RMS value of the data. This measure was then evaluated in the window from 60- to 145-msec poststimulus by searching for local minima in 5-msec blocks and then discarding all but the two lowest values (i.e., these are the latencies when the ECD best modeled the data). Mean latencies were 77611 msec poststimulus for the early

source and 100 6 11 msec for the late source. We have

previously reported that the two sources, so determined, were significantly different from one another. Additional details are provided in Teale et al (1998).

Statistical Procedures

All statistical analyses were performed using Statistica 5.5 (StatSoft, Tulsa OK). Analyses were conducted usinga 5.05.

Sums of squares for all analyses of variance designs were type III. We employed a 33232 analysis of variance (ANOVA;

group by hemisphere by source latency), with hemisphere and source latency treated as repeated measures and y location of the sources as the dependent variable, to test differences in source location. To examine our hypothesis concerning schizophrenia

and schizoaffective disorder, two orthogonal interaction contrasts were coded within this ANOVA to test 1) whether the schizoaf-fective and schizophrenia groups, when combined together, differed from the control group and 2) whether the schizophrenia group and schizoaffective group differed from each other.

Results

The first contrast was significant [

F

(1,46)

5

4.03,

p

,

.05], indicating that schizophrenic and schizoaffective

subjects differed from control subjects. The second

con-trast was nonsignificant [

F

(1,46)

5

0.03,

p

.

.05],

indicating that schizoaffective and schizophrenic patients

did not differ significantly from each other in overall

source location. In control subjects, the second source was

more lateralized than the first [

F

(1,46)

5

3.76,

p

,

.06].

The early and late sources were not lateralized in either

patient group [

F

(1,46)

5

0.03,

p

.

.05]. Figure 1

illustrates the mean anteroposterior dipole locations for

each group for the early and late source.

Discussion

Our findings suggest the second subcomponent could be a

major contributing factor to the laterality differences

previously reported for the combined M100 in

schizophre-nia. Thus, experimental demands, or signal processing

differences that inadvertently emphasize one of the two

subcomponents, could influence the laterality differences

reported in the literature. Low-pass filtering, for example,

would likely preferentially emphasize the subcomponent

with the highest amplitude (assuming the subcomponents

are similar in waveform) and so shift source parameter

estimates. A recent report by Rockstroh and colleagues

(Rockstroh et al 1998) demonstrated a failure in the

development of contralateral dominance in patients with

schizophrenia as indexed by M100 ECD strength. Source

estimates, however, did not differentiate between control

subjects and patients with respect to left–right, anterior–

posterior location. In this case, data were low-pass filtered

at 20 Hz. Consideration of a two source model might

produce a larger difference in these parameters.

Anomalous lateralization of the M100 component

pre-viously described in patients with schizophrenia has been

suggested to reflect evidence of a different cortical

orga-nization in schizophrenia (Rojas et al 1997). The present

findings do not directly address the issue of cortical

organization but suggest that such work might profitably

include independent consideration of the several

subcom-ponents contributing to the M100. Schizophrenic subjects

did not differ from subjects with schizoaffective disorder

on this metric, implicating a commonality of the temporal

lobe pathology in the schizophreniform psychoses.

Sub-1110 BIOL PSYCHIATRY P. Teale et al

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jects with affective psychoses have yet to be studied in this

regard.

The M100 complex has previously been associated with

auditory sensory memory or echoic memory (Imada et al

1993; Lu et al 1992; Sams et al 1993). Lu et al (1992)

suggested that two components of the M100 complex,

what they termed L100m (an earlier, posterior component)

and N100m (a later, more anterior component) had

differ-ent trace lifetimes and suggested differdiffer-ent functional roles

for each source. In a later paper, Sams et al (1993) also

observed two sources underlying the M100 complex,

which they termed N100m

p

and N100m

a

(early posterior

and later anterior, respectively). Sams et al (1993) also

observed differing trace decays for the two sources, with

the N100m

p

exhibiting shorter time constant of decay than

the N100m

a

, in agreement with the findings of Lu et al

(1992). Loveless et al (1996) suggested that these two

sources might reflect the short and long term auditory

stores first proposed by Strous and colleagues (Strous et al

1995) on the basis of behavioral data. Our data indicate

that the differences between the control group and two

psychotic groups are largely confined to the later source

(N100m

a

), suggesting an impairment in the longer term

auditory store. By implication, experimental paradigms

with different memory demands may preferentially

acti-vate one subcomponent. If, for example, the amplitude of

one was increased, the apparent localization of the

com-bined source might appear to move forward or backward.

It might be important to determine the extent to which

attentional mechanisms may be involved in the activation

of the second course. Such mechanisms, thought to be

disturbed in schizophrenia, might preferentially alter

strength of location of this source. Clearly, there are

concerns relating to the variable nomenclature of these

auditory evoked field components, which to date, in the

absence of agreed upon terminology, tend to be laboratory

specific. We hope our discussion will help relate the

somewhat varying nomenclatures.

One caveat in considering these findings is that they are

based on a sequential source model. Improvements in the

accuracy of localization might be obtained with the

appli-cation of a true two-source model in the time window

during which both sources are active. This might involve

a two-pass modeling strategy wherein the first pass would

be as reported here and the second pass would involve a

pair of simultaneously active spatiotemporal ECDs

cover-ing the latency window between the two sources identified

in pass one.

This work was supported by National Institute of Mental Health Grant No. MH47476.

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Fine Structure of the Auditory M100 BIOL PSYCHIATRY 1111

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1112 BIOL PSYCHIATRY P. Teale et al

Gambar

Figure 1. Mean anteroposterior M100

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