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Volumn 130, Issue 16, 2009, Pages

Phase-resolved two-dimensional spectroscopy based on collinear n -wave mixing in the ultrafast time domain

Author keywords

[No Author keywords available]

Indexed keywords

2D SPECTRUM; COLLINEAR BEAMS; DIFFERENT ORDERS; ELECTRO-OPTIC SAMPLINGS; FEMTOSECOND; FOURIER; GAAS/ALGAAS; INTER-SUBBAND TRANSITIONS; MID-INFRARED; MULTIPLE QUANTUM WELLS; NON-LINEAR RESPONSE; NONLINEAR SIGNALS; REAL TIME; TIME DOMAINS; TWO PHASE; ULTRA FASTS; VARIABLE TIME DELAYS; WAVE MIXING;

EID: 65149095750     PISSN: 00219606     EISSN: None     Source Type: Journal    
DOI: 10.1063/1.3120766     Document Type: Article
Times cited : (127)

References (31)
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    • If necessary, one can easily extend the method to more than two pulses. Independently chopping all pulses, one can extract the nonlinear signal analogous to Eq.
    • If necessary, one can easily extend the method to more than two pulses. Independently chopping all pulses, one can extract the nonlinear signal analogous to Eq.
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    • The nonlinear signal is a real quantity and, thus, the Fourier transform is invariant against the simultaneous sign change in t and τ (cf. Fig.). Therefore the first pump-probe signal will also occur at t =- 0 and τ = 0.
    • The nonlinear signal is a real quantity and, thus, the Fourier transform is invariant against the simultaneous sign change in t and τ (cf. Fig.). Therefore the first pump-probe signal will also occur at t =- 0 and τ = 0.
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    • The sensitivity of our electro-optic setuis limited to frequencies t 40 THz by the 12 fs duration of the 800 nm sampling pulses, thus setting an upper limit for the detection in t. In τ, the much higher frequency limit is determined by the stepsize used in scanning the delay.
    • The sensitivity of our electro-optic setup is limited to frequencies t 40 THz by the 12 fs duration of the 800 nm sampling pulses, thus setting an upper limit for the detection in t. In τ, the much higher frequency limit is determined by the stepsize used in scanning the delay τ.


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