... CCAATGCAGTCTATTTCCCTAG AGCCGCAATCAGACTTCG CGTCAACAGTCGCCTTCAGG GCCGATGGCATTGACATTG TACCGCACAACAAAAGGGA TCTTTTAGTTCCAGGAACCTG AAGAAGACCTGGGGCTGGA ATGTAGATGATGTAGTCGAC GTATCTCAAGGGATTCCCCA GAATTCTTCTATCAACGAGAGG ... GACTCTCGAGATCAAGCAC TCTGATTGCGGCTGGTTTC GCAATTGAGAGCAGTTTCG TTGAAGAAGGAGCACGAATGCC AAGAGAAGAGATGGTGGTCC CTCTCACCATCAAAGCCAAAG TCATGTCTAAGAGCATAGGC TGTCCAGTTGCCCGAGTTGA CGGGCTATCTGAT...
Ngày tải lên: 07/03/2014, 12:20
... dot dimensions are smaller than the effective Bohr radius, we show that this interaction affects the excitonic effects of the secondorder nonlinear optical properties of semi-spherical quantum dots ... K-X: Exciton effects on the nonlinear optical rectification in one-dimesional quantum dots Phys Lett A 2005, 335:175 Baskoutas S, Paspalakis E, Terzis AF: E...
Ngày tải lên: 21/06/2014, 04:20
OPTICAL IMAGING AND SPECTROSCOPY Phần 1 pdf
... Present, and Future xvii 1. 1 Three Revolutions / 1. 2 Computational Imaging / 1. 3 Overview / 1. 4 The Fourth Revolution / Problems / Geometric Imaging 11 2 .1 Visibility / 11 2.2 Optical Elements / 14 ... Figure 2 .11 Refraction by a parabolic surface a, that g % 1, we obtain n2 À (n1 À n2 ) R2 R2 ¼ n1 À n1 R1 F (2 :15 ) or ¼ F n2 1 1 À R1 R2 n1 Figure 2 .12 Focus...
Ngày tải lên: 05/08/2014, 14:20
OPTICAL IMAGING AND SPECTROSCOPY Phần 2 ppt
... L 2( R) and g(x) [ L 2( R) ð ^Ã (u)^(u) du ¼ g f À1 ð f Ã(x)g(x)dx (3 :20 ) À1 Localization Defining mf ¼ s2 f ¼ ð jj f jj xj f (x)j2 dx (3 :21 ) (x À mf )2 j f (x)j2 dx (3 :22 ) ^ uj f (u)j2 du (3 :23 ) ... sf2 sf ^2 ¼ ^ jj f jj jj f jj2 ð ð À1 À1 ^ x2 j f (x)j2 (u À mf^ )2 j f (u)j2 dx du (3 :26 ) 62 ANALYSIS Combining Eqns (3.14) and (3.19), we note that ð j2pixf (x)j dx ¼ À1 ð À1...
Ngày tải lên: 05/08/2014, 14:20
OPTICAL IMAGING AND SPECTROSCOPY Phần 3 potx
... PROBLEMS 3. 1 Fourier Uncertainty Show that for f (x) ¼ aeÀb(xÀxo ) sf2 s ^ ¼ f 16p (3: 165) 3. 2 3. 3 Fourier Rotation Derive Eqn (3. 39) Fresnel Identities: (a) Derive Eqn (3. 63) (b) Derive Eqn (3. 64) 3. 4 ... Figs 3. 9, 3. 12, and 3. 17 for your function 3. 11 2D Wavelet Analysis Replicate Figs 3. 13 and 3. 14 for an image of your choosing 3. 12 Spline Interpolation: (a)...
Ngày tải lên: 05/08/2014, 14:20
OPTICAL IMAGING AND SPECTROSCOPY Phần 4 docx
... irradiance-based imaging and spectroscopy (which is to say, essentially all optical imaging and spectroscopy) The enormous disparity between the oscillation frequency of the optical field and the temporal ... objectives of this chapter are to Optical Imaging and Spectroscopy By David J Brady Copyright # 2009 John Wiley & Sons, Inc 147 148 † † † DETECTION Motivate and...
Ngày tải lên: 05/08/2014, 14:20
OPTICAL IMAGING AND SPECTROSCOPY Phần 5 ppsx
... ! x1 þ 0:5a x2 þ 0:5a þ fo fo 2^ a 2^ a ¼ S(n)[2jfÀ ihfÀ j þ jfþ ihfþ j] (6:1 05) where fo (x) is the fundamental Gaussian mode of Eqn (3 .55 ), jfÀ i ¼ fo ( y=2a)fo [(x À 0:5a)=2a)] and jfþ i ... bandwidth product and the etendue of an optical system The space – bandwidth product is the product of the spatial support over which an optical signal is observed and the spatial frequen...
Ngày tải lên: 05/08/2014, 14:20
OPTICAL IMAGING AND SPECTROSCOPY Phần 6 potx
... system and the spectral resolution necessary to operate it 6. 10 Resolution and 3D Imaging Section 6. 4.2 uses dux % l=A and dz % 8lz2 =A2 to approximate the angular and range resolution for 3D imaging ... imaging using Eqn (6. 73) Derive and explain these limits Compare the resolution of this approach with projection tomography and optical coherence tomography 6. 11 Ba...
Ngày tải lên: 05/08/2014, 14:20
OPTICAL IMAGING AND SPECTROSCOPY Phần 7 potx
... transmission, and reflection may arise in optical devices and materials as a result of microscopic optical and electronic properties rather than macroscopic optical design Resonant effects are created by optical ... matrix (b) A random 1 27 1 27 matrix with values uniformly drawn from [21, 1] (c) The level Haar wavelet transform of f 8.3 Regularizaton Operating from the left an...
Ngày tải lên: 05/08/2014, 14:20
OPTICAL IMAGING AND SPECTROSCOPY Phần 8 pptx
... (9 :87 ) At normal incidence with n2 d2 ¼ n1 d1 ¼ d, for example, the edges of the stopband occur at l such that cos2 2pd 2pd n1 n2 þ À sin2 ¼ +1 l l n2 n1 (9 :88 ) Solutions to Eqn (9 .88 ) ... application in spectroscopy will greatly expand In particular, two- and three-dimensional resonant filters, as discussed in Section 9 .8, greatly increase the power of this technology ...
Ngày tải lên: 05/08/2014, 14:20
OPTICAL IMAGING AND SPECTROSCOPY Phần 9 doc
... resolution, and field of view In practice, however, optical system performance is limited by both aperture size and the capabilities of optical and optoelectronic processing to condition and extract ... components are u ¼ Dx=l and v ¼ Dy=l The longitudinal frequency is w ¼ q=l The bandpass is determined by the limits of Dx, Dy, and q within the aperture and cannot be increase...
Ngày tải lên: 05/08/2014, 14:20
OPTICAL IMAGING AND SPECTROSCOPY Phần 10 doc
... Naulleau and E Leith, Imaging through optical fibers by spatial coherence encoding methods, J Opt Soc Am A 13 (10) :2096 – 2101 , 1996 185 M A Neifeld and J Ke, Optical architectures for compressive imaging, ... =100 for l ¼ 1mm for 100 mm , z0 , 100 m Assuming that A ¼ 100 mm, plot the aperture displacement necessary to achieve similar longitudinal resolution using optical pro...
Ngày tải lên: 05/08/2014, 14:20
Nonlinear photonic crystals a study of the microstructure designs parametric processes
... description of these processes The physical interpretation of SFM is straightforward The laser beams at frequencies of ω1 and ω interact in a nonlinear optical crystal and generate a nonlinear polarization ... in nonlinear optics is the study of parametric process in nonlinear optical materials The parametric process has been systematically investigated and...
Ngày tải lên: 14/09/2015, 13:11