2009
DOI: 10.1063/1.3184103
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A versatile ultrastable platform for optical multidimensional Fourier-transform spectroscopy

Abstract: The JILA multidimensional optical nonlinear spectrometer (JILA-MONSTR) is a robust, ultrastable platform consisting of nested and folded Michelson interferometers that can be actively phase stabilized. This platform generates a square of identical laser pulses that can be adjusted to have arbitrary time delay between them while maintaining phase stability. The JILA-MONSTR provides output pulses for nonlinear excitation of materials and phase-stabilized reference pulses for heterodyne detection of the induced s… Show more

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Cited by 176 publications
(153 citation statements)
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References 36 publications
(45 reference statements)
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“…The experimental setup, shown in Fig. 2, is based on three-pulse transient FWM with the addition of interferometric stabilization of the pulse delays [26]. 150-fs pulses with wave vectors k a , k b and k c are focused onto the sample to generate a FWM signal in the direction k s = −k a + k b + k c .…”
Section: Optical 2d Fourier-transform Spectroscopymentioning
confidence: 99%
“…The experimental setup, shown in Fig. 2, is based on three-pulse transient FWM with the addition of interferometric stabilization of the pulse delays [26]. 150-fs pulses with wave vectors k a , k b and k c are focused onto the sample to generate a FWM signal in the direction k s = −k a + k b + k c .…”
Section: Optical 2d Fourier-transform Spectroscopymentioning
confidence: 99%
“…In particular, in the optical frequency range minute mechanical drifts can lead to significant phase drifts comparable to the wavelength that would lead to inadequate 2DFT spectra. However, instrumentation developed recently consisting of an ultrastable platform of nested and folded Michelson interferometers that can be actively phase stabilized can overcome these challenges 5 . The advantages of multidimensional spectroscopy are well documented in the literature 6 .…”
mentioning
confidence: 99%
“…Although not the most straightforward to implement, the 'box' geometry [15,31,32,33,34,35] ( Fig. 8 (a)) is versatile and conceptually easy to understand.…”
Section: Box Geometrymentioning
confidence: 99%
“…This direction ensures that pulse A is acting as the conjugate pulse in the sequence. Rephasing, nonrephasing or two-quantum signals can be selectively obtained by having the conjugated pulse A * arriving on the sample in the first, second or third position [15,34,35]. The signal is spectrally resolved by a grating-based spectrometer on a CCD camera -providing, in a single acquisition, the Fourier transform of the signal with respect to emission time t. Phase resolution is obtained through spectral interferometry [36], where the signal is heterodyned with a reference pulse (local oscillator (LO)).…”
Section: Box Geometrymentioning
confidence: 99%