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fMRI Noise Problems and Methods to Mitigate

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There is equal energy in all octaves (or similar log bundles)[3] ... In terms of power at a constant bandwidth, 1/f noise falls off at 3dB per octave[3] ... – PowerPoint PPT presentation

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Title: fMRI Noise Problems and Methods to Mitigate


1
fMRI Noise Problems and Methods to Mitigate
  • Presented by
  • Clay McCreary

2
Introduction
  • Noise can affect an fMRI imaging session in two
    ways
  • Creates artifacts in the image
  • Strong acoustic noise interferes with the audio
    stimuli (talking to the patient) used in imaging
    experiments, and creates a harmful, annoying
    environment for both the patient and the
    staff4.

3
Creating Artifacts
  • Drift Noise
  • Reference 1 defines drift as low frequency
    signal that varies slowly across the whole period
    of the acquisition of the data caused by12
  • Gross head motion
  • Cerebrospinal fluid (CSF) pulsations
  • Physiological fluctuations
  • Local Magnetic susceptibility changes
  • Image Noise
  • Reference 1 has determined through observation
    that the noise in fMRI has the characteristics of
    fractional noise and exhibits long range
    autocorrelation in time.

4
Fractional Noise
  • Sometimes referred to as Pink Noise3
  • Signal or process with a frequency spectrum such
    that the power spectral density is proportional
    to the reciprocal of the frequency3.
  • There is equal energy in all octaves (or similar
    log bundles)3.
  • White noise has equal energy per hertz3
  • In terms of power at a constant bandwidth, 1/f
    noise falls off at 3dB per octave3.

5
Modeling Drift Noise
  • Drift noise is assumed to vary slowly with large
    scales1.
  • A discrete wavelet transform is used to model
    drift noise1
  • Fine scale wavelet coefficients will be zero
    since drift noise is low frequency and thus does
    not vary greatly over a short period of time.

6
Modeling Image and Acoustic Noise
  • The image noise in the fMRI time series obtained
    under the resting or null conditions exhibit
    long-range autocorrelation in time and 1/f-like
    spectral properties (fractional noise)1.
  • Acoustic noise is AWGN.
  • Generated by the rapid switching of the scanner
    coil to produce the strong magnetic field gradient

7
Methods to Solve Noise Problem
  • Modified General Linear Model and Bayesian
    Estimator1
  • Blind Dereverberation for fMRI Noise Based on
    SIMO Linear Prediction Method4
  • LMS-based Active Noise Cancellation Methods for
    fMRI Using Sub-band Filtering5

8
Modified General Linear Model and Bayesian
Estimator1
  • Discrete wavelet decomposition is applied to the
    signal.
  • yi ßbi fi ni, i 1, . . . , N (assumed LTI)
  • yi is the fMRI signal at a specific voxel
  • ß is a scalar estimation of the contribution of
    the desired signal to yi
  • fi is the contribution of drift to yi
  • ni is the contribution of noise to yi

9
Modified General Linear Model and Bayesian
Estimator1 (cont)
  • Since fi is present only in large scale wavelets,
    finer scales are used for this calculation
    removing this term.
  • Applying an orthonormal wavelet process
    decorrelates the noise and the wavelet
    coefficients are normally distributed with zero
    mean and identical variances at the same
    levels1.
  • Bayesian estimator accurately determines the
    noise covariance matrix thus ß is accurately
    determined.

10
Blind Dereverberation for fMRI Noise Based on
SIMO Linear Prediction Method4
  • Active noise cancellation (ANC) is used to
    mitigate acoustic noise
  • Room reverberation degrades the performance of
    the ANC
  • This method models the room as a single input
    multiple output (SIMO) system using two
    microphones to capture some of the reverberation
    from the room.

11
Blind Dereverberation for fMRI Noise Based on
SIMO Linear Prediction Method4(cont)
  • An algorithm based on a prediction method to
    reduce the reverberation from the two
    microphones output is used on the SIMO
    system4.
  • The output of the microphones correlates with the
    entire room reverberation.
  • The room reverberation is predicted and cancelled
    without the room transfer function.

12
LMS-based Active Noise Cancellation Methods for
fMRI Using Sub-band Filtering5
  • Using a least mean squared (LMS) finite impulse
    response (FIR) filter over the entire band of
    acoustic noise produced by the fMRI will result
    in a heavy computational load and significant
    time delay.

13
LMS-based Active Noise Cancellation Methods for
fMRI Using Sub-band Filtering5(cont)
  • Dividing the acoustic band into subbands and
    implementing LMS-FIR filters on each subband then
    combining them using a stacking method allows
    for less computational load and nearly real time
    results.
  • Since the subband method is essentially
    delayless it provides a more effective means of
    ANC.

14
References
  • 1 Huaien Luo and Sadasivan Puthusserypady,
    Analysis of fMRI Data With Drift Modified
    General Linear Model and Bayesian Estimator,
    IEEE TRANSACTIONS ON BIOMEDICAL ENGINEERING, VOL.
    55, NO. 5, pp. 1504-1511, May 2008
  • 2 T. Kim, L. Al-Dayeh, and M. Singh, FMRI
    Artifacts Reduction Using Bayesian Image
    Processing, IEEE TRANSACTIONS ON NUCLEAR
    SCIENCE, VOL. 46, NO. 6, pp. 2134-2140, DECEMBER
    1999

15
References (cont)
  • 3 Wikipedia, Pink Noise, Retrieved from the
    world wide web, June 7, 2008 from
    http//en.wikipedia.org/wiki/1/f_noise
  • 4 Hua Bao, Issa M.S. Panahi, Richard Briggs,
    Blind Dereverberation for fMRI Noise Based on
    SIMO Linear Prediction Method, Proceedings of
    the 29th Annual International Conference of the
    IEEE EMBS Cité Internationale, Lyon, France, pp.
    2831-2834, 2007

16
References (cont)
  • 5 Ali A. Milani, Student Member. Issa Panahi,
    Richard Briggs, LMS-based Active Noise
    Cancellation Methods for fMRI Using Sub-band
    Filtering, Proceedings of the 28th IEEE EMBS
    Annual International Conference New York City,
    USA, pp. 513-516, Aug 30-Sept 3, 2006
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