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翻訳と辞書　辞書検索 [ 開発暫定版 ] スポンサード リンク MIIPS ： ウィキペディア英語版 Multiphoton intrapulse interference phase scan Multiphoton intrapulse interference phase scan (MIIPS) is a method used in ultrashort laser technology that simultaneously measures (phase characterization), and compensates (phase correction) femtosecond laser pulses using an adaptive pulse shaper. Current ultrashort laser pulse characterization methods (streak camera, autocorrelation, FROG, SPIDER etc.) can only measure the pulse characteristics. Thus, the application of an ultrashort pulse is limited as the electromagnetic field of a pulse is determined by the laser cavity, and varies dramatically when the pulse duration is in the femtosecond region. It is therefore highly desirable to have a method which can not only characterize the pulse, but also correct the pulse to specific shapes for various applications in which repeatable pulse characteristics are requested. MIIPS can not only measure the pulse but also correct the high-order dispersion, thus is highly preferable for applications where repeatable electromagnetic field is important, such as to generate ultrashort pulses which are transform limited or possess specific phase characteristics. ==Theory== A MIIPS-based device consists of two basic components controlled by a computer: a pulse shaper (usually a liquid crystal based spatial light modulator - SLM) and a spectrometer. The pulse shaper allows manipulation of the spectral phase and/or amplitude of the ultrashort pulses. The spectrometer records the spectrum of a nonlinear optical process such as second harmonic generation produced by the laser pulse. The MIIPS process is analogous to the Wheatstone bridge in electronics. A well-known (calibrated) spectral phase function is used in order to measure the unknown spectral phase distortions of the ultrashort laser pulses. Typically, the known superimposed function is a periodic sinusoidal function that is scanned across the bandwidth of the pulse. MIIPS is similar to FROG in that a frequency trace is collected for the characterization of the ultrashort pulse. In Frequency-resolved optical gating, a FROG trace is collected through scanning the ultrashort pulse across the temporal axis, and detecting the spectrum of the nonlinear process. It can be expressed as :$$ I(\omega,\tau)=\left|\intt}\right|^2 In MIIPS, instead of scanning on the temporal domain, a series of phase scan is applied on the phase domain of the pulse. The trace of the MIIPS scan consists of the second-harmonic spectra of each phase scan. The signal of MIIPS can be written as :$$ I(2\omega)=\left|\int\phi}\right|^2 The phase scan in MIIPS is realized with introducing a well-known reference function, $f(\backslash omega)$, by the pulse shaper to locally cancel distortions by the unknown spectral phase, $\backslash Phi(\backslash omega)$, of the pulse. The sum of the unknown phase and the reference phase is given by $\backslash phi(\backslash omega)=\backslash Phi(\backslash omega)+\; f(\backslash omega)$. Because the frequency doubled spectrum of the pulse depends on $\backslash phi(\backslash omega)$, it is possible to accurately retrieve the unknown $\backslash Phi(\backslash omega)$. The phase modulation procedure of the physical process is generally a continuous function. Thus, the SHG signal can be expanded with a Taylor expansion around $\backslash omega$: :$$ I(\omega)= \left| \int| E(\omega+\Omega)| |E(\omega-\Omega)| \times \text \ \mathrm\Omega \right|^2 And :$$ \phi(\omega+\Omega)+\phi(\omega-\Omega)=2\phi0+\phi''(\omega)\Omega^2+...+\frac\phi^(\omega)\Omega^ According to this equation, the SHG signal reaches maximum when $\backslash phi(\backslash omega+\backslash Omega)+\backslash phi(\backslash omega-\backslash Omega)$ is zero. This is equivalent to $\backslash Phi\text{'}\text{'}(\backslash omega)=-f\text{'}\text{'}(\backslash omega)$. Through scanning of $f(\backslash omega)$, the $\backslash Phi(\backslash omega)$ can be decided. The frequency doubled spectrum recorded for each full scan of the reference phase $4(\backslash pi)$ results in two replicas of the MIIPS trace (see Figure 1, four replicas shown). From this data, a 2D plot for SHG($\backslash omega,\backslash omega$) is constructed where $\backslash omega=\backslash pi\; c/\backslash lambda\_$. The second harmonic spectrum of the resulting pulse has a maximum amplitude at the frequency where the second derivative of the pulse has been compensated. The lines describing $\backslash omega\_(\backslash omega)$ are used to obtain analytically the second derivative of the unknown phase. After double integration the phase distortions are known. The system then introduces a correction phase to cancel the distortions and achieve shorter pulses. The absolute accuracy of MIIPS improves as the phase distortions diminish, therefore an iterative procedure of measurement and compensation is applied to reduce phase distortions below 0.1 radian for all frequencies within the bandwidth of the laser. When all phase distortions have been eliminated, the pulses are the shortest they can be and are considered to be Bandwidth-limited-pulse|transform limited (TL). The MIIPS trace corresponding to TL pulses shows straight parallel lines separated by $\backslash pi$. Once spectral phase distortions have been eliminated, the shaper can be used to introduce calibrated phases and amplitudes to control laser induced processes. MIIPS technology has been applied successfully in selective excitation of multiphoton imaging and femtosecond light-mass interaction study. 抄文引用元・出典: フリー百科事典『 ウィキペディア（Wikipedia）』 ■ウィキペディアで「Multiphoton intrapulse interference phase scan」の詳細全文を読む スポンサード リンク 翻訳と辞書 : 翻訳のためのインターネットリソース Copyright(C) kotoba.ne.jp 1997-2016. All Rights Reserved.