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Ryohei's Neuroscience Notes

Tuesday, December 19, 2006. Group velocity dispersion memo. Mode-lock pulsed laser has broad wavelength spectrum due to the Heisenberg principle:. Δν τ = τ cΔλ/(λ. 044 (FWHM). For 100fs, the wavelength width (Δλ) is 8nm at 800nm wavelength. Because light with different wavelength propagates with different velocity, the dispersion of pulsewidth occurs. Phase shift of light in some material is:. Φ (ω) = n(ω)Lω/c (1). Compensation can be done using a pair of prism with distance of L. A1,A2,A3,B1,B2,B3.

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Ryohei's Neuroscience Notes | ryasuda.blogspot.com Reviews
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Tuesday, December 19, 2006. Group velocity dispersion memo. Mode-lock pulsed laser has broad wavelength spectrum due to the Heisenberg principle:. Δν τ = τ cΔλ/(λ. 044 (FWHM). For 100fs, the wavelength width (Δλ) is 8nm at 800nm wavelength. Because light with different wavelength propagates with different velocity, the dispersion of pulsewidth occurs. Phase shift of light in some material is:. Φ (ω) = n(ω)Lω/c (1). Compensation can be done using a pair of prism with distance of L. A1,A2,A3,B1,B2,B3.
<META>
KEYWORDS
1 ryohei's neuroscience notes
2 φ ω = φ ω
3 dφ ω /dω ω ω
4 φ ω /dω
5 n/dλ
6 cδλ / λ
7 prism
8 obtained by
9 dn/dλ
10 sellmeier equation
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ryohei's neuroscience notes,φ ω = φ ω,dφ ω /dω * ω ω,φ ω /dω,n/dλ,cδλ / λ,prism,obtained by,dn/dλ,sellmeier equation,references,newport web page,mellesgriot web page,wikipedia sellmeier equation,bcp webpage,materials,frap and fdap,exp x,erf{ x b/2 / 4dt
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Ryohei's Neuroscience Notes | ryasuda.blogspot.com Reviews

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Tuesday, December 19, 2006. Group velocity dispersion memo. Mode-lock pulsed laser has broad wavelength spectrum due to the Heisenberg principle:. Δν τ = τ cΔλ/(λ. 044 (FWHM). For 100fs, the wavelength width (Δλ) is 8nm at 800nm wavelength. Because light with different wavelength propagates with different velocity, the dispersion of pulsewidth occurs. Phase shift of light in some material is:. Φ (ω) = n(ω)Lω/c (1). Compensation can be done using a pair of prism with distance of L. A1,A2,A3,B1,B2,B3.

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1

Ryohei's Neuroscience Notes: Group velocity dispersion memo

http://ryasuda.blogspot.com/2006/12/group-velocity-dispersion-memo.html

Tuesday, December 19, 2006. Group velocity dispersion memo. Mode-lock pulsed laser has broad wavelength spectrum due to the Heisenberg principle:. Δν τ = τ cΔλ/(λ. 044 (FWHM). For 100fs, the wavelength width (Δλ) is 8nm at 800nm wavelength. Because light with different wavelength propagates with different velocity, the dispersion of pulsewidth occurs. Phase shift of light in some material is:. Φ (ω) = n(ω)Lω/c (1). Compensation can be done using a pair of prism with distance of L. A1,A2,A3,B1,B2,B3.

2

Ryohei's Neuroscience Notes: February 2005

http://ryasuda.blogspot.com/2005_02_01_archive.html

Monday, February 14, 2005. Neurons to make decision. Optical Imaging of Neuronal Populations During Decision-Making. Posted by Ryohei at 12:29 PM. Thursday, February 10, 2005. Calcium imaging to analyze circuit. Functional imaging with cellular resolution reveals precise micro-architecture in visual cortex. 2005), Ohki K. et al.Nature 433, 597 - 603 (Reid lab.). Posted by Ryohei at 1:07 PM. View my complete profile. Group velocity dispersion memo. Building a 2-photon microscope - 2.

3

Ryohei's Neuroscience Notes: Effects of coverslip on PSF

http://ryasuda.blogspot.com/2005/01/effects-of-coverslip-on-psf.html

Thursday, January 20, 2005. Effects of coverslip on PSF. We use water-dip type objective for our two-photon microscopy. However, if there is a coverslip between the objective and the sample, the PSF(Point spread function) is degraded significantly. This is because the these objectives are not designed for this situation. Can be calculated as:. Where N/N' = sinθ / sinθ' (N: refractive index of water, N': of coverslip), and a. Is coverslip thickness (typically 170 μm). In this case the shift D.

4

Ryohei's Neuroscience Notes: Calcium imaging to analyze circuit

http://ryasuda.blogspot.com/2005/02/calcium-imaging-to-analyze-circuit.html

Thursday, February 10, 2005. Calcium imaging to analyze circuit. Functional imaging with cellular resolution reveals precise micro-architecture in visual cortex. 2005), Ohki K. et al.Nature 433, 597 - 603 (Reid lab.). The column structure in the cortex has fascinated many brain researchers: why are cells that response to similar stimulations clustered to form a column? Posted by Ryohei at 1:07 PM. View my complete profile. Spine structural change - Nothing to do with physi. Effects of coverslip on PSF.

5

Ryohei's Neuroscience Notes: January 2005

http://ryasuda.blogspot.com/2005_01_01_archive.html

Friday, January 28, 2005. Spine structural change - Nothing to do with physiology? Today's journal club was about Shrinkage of dendritic spines associated with LTD, Neuron. 2004 Dec 2;44(5):749-57. Clearly spine structural change is NOT required by the change in synaptic strength. This is probably the same for LTP and spine enlargement: I heard from several guys that the washout by patch-clamping often blocks selectively the spine enlargement but not LTP. Then why the spine structure changes? For analysi...

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Daily Crumbs: August 2005

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Everyday, about 10,000 neurons die per brain. These are daily crumbs falling out of my head. These are Rantings. This is a tribute to my favorite instant noodles - Chu Qian Yi Ding, which I always miss dearly when I am away from home. Wednesday, August 31, 2005. Be careful what you wish for. Fulfilment of Wish List. only 1 item Yes, I am now employed. I guess this paves the way for the rest of my wishes. A part of me simply cringe whenever I see that. Its the yunshi-effect. Posted by eline @ 1:56 AM.

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Tuesday, December 19, 2006. Group velocity dispersion memo. Mode-lock pulsed laser has broad wavelength spectrum due to the Heisenberg principle:. Δν τ = τ cΔλ/(λ. 044 (FWHM). For 100fs, the wavelength width (Δλ) is 8nm at 800nm wavelength. Because light with different wavelength propagates with different velocity, the dispersion of pulsewidth occurs. Phase shift of light in some material is:. Φ (ω) = n(ω)Lω/c (1). Compensation can be done using a pair of prism with distance of L. A1,A2,A3,B1,B2,B3.

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