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Published byAmie Wheeler Modified over 8 years ago
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Lecture 23: 1. MRI noise processes MP574
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Dipole Moments from Entire Sample Magnetic Field (B 0 ) Positive Orientation Negative Orientation Magnetic Field (B 0 )
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Source of Signal Proton or Water MRI –B o Magnetic Field –Proton Nucleus S = ±ħ/2 EE oz B kT ME 4 22
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Detected Signal )sin() )()( )cos( 2 1 tg kT Ah tg kT BAh tStV tgAB L L LL o L x y z B 1 (t)
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Brownian Motion http://en.wikipedia.org/wiki/Wiener_process Brownian Motion Conditions: x 0 = 0 x(t) is a continuous random variable Increments x(t 1 ) and x(t 2 ) are statistically independent and normally distributed
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Brownian Motion
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Johnson or “Thermal” Noise RpRp RcRc Patient Resistance Electrical Resistance of Coil Thermal noise in patient dominant at high field strengths
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Johnson or “Thermal” Noise on both I and Q channels I = “in phase” Q = “quadrature” or 90 o out of phase Imaginary Real
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Independent Realizations of GWN on each of the I,Q channels Imaginary Real
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Background noise Imaginary Real
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Rayleigh and Rician Probability Distribution Functions
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High SNR
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Dependence on SNR
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