High-Order Harmonics of Bichromatic Counter-Rotating Elliptically-Polarized Drivers: Fully Controlled Polarization State and Novel Selection Rules

Author(s):  
Avner Fleischer ◽  
Pavel Sidorenko ◽  
Oren Cohen
2016 ◽  
Vol 194 ◽  
pp. 161-183 ◽  
Author(s):  
K. Veyrinas ◽  
V. Gruson ◽  
S. J. Weber ◽  
L. Barreau ◽  
T. Ruchon ◽  
...  

Due to the intimate anisotropic interaction between an XUV light field and a molecule resulting in photoionization (PI), molecular frame photoelectron angular distributions (MFPADs) are most sensitive probes of both electronic/nuclear dynamics and the polarization state of the ionizing light field. Consequently, they encode the complex dipole matrix elements describing the dynamics of the PI transition, as well as the three normalized Stokes parameters s1, s2, s3 characterizing the complete polarization state of the light, operating as molecular polarimetry. The remarkable development of advanced light sources delivering attosecond XUV pulses opens the perspective to visualize the primary steps of photochemical dynamics in time-resolved studies, at the natural attosecond to few femtosecond time-scales of electron dynamics and fast nuclear motion. It is thus timely to investigate the feasibility of measurement of MFPADs when PI is induced e.g., by an attosecond pulse train (APT) corresponding to a comb of discrete high-order harmonics. In the work presented here, we report MFPAD studies based on coincident electron-ion 3D momentum imaging in the context of ultrafast molecular dynamics investigated at the PLFA facility (CEA-SLIC), with two perspectives: (i) using APTs generated in atoms/molecules as a source for MFPAD-resolved PI studies, and (ii) taking advantage of molecular polarimetry to perform a complete polarization analysis of the harmonic emission of molecules, a major challenge of high harmonic spectroscopy. Recent results illustrating both aspects are reported for APTs generated in unaligned SF6 molecules by an elliptically polarized infrared driving field. The observed fingerprints of the elliptically polarized harmonics include the first direct determination of the complete s1, s2, s3 Stokes vector, equivalent to (ψ, ε, P), the orientation and the signed ellipticity of the polarization ellipse, and the degree of polarization P. They are compared to so far incomplete results of XUV optical polarimetry. We finally discuss the comparison between the outcomes of photoionization and high harmonic spectroscopy for the description of molecular photodynamics.


2007 ◽  
Vol 99 (24) ◽  
Author(s):  
Jérôme Levesque ◽  
Yann Mairesse ◽  
Nirit Dudovich ◽  
Henri Pépin ◽  
Jean-Claude Kieffer ◽  
...  

2021 ◽  
Vol 5 (1) ◽  
Author(s):  
Kotaro Nakagawa ◽  
Hideki Hirori ◽  
Yasuyuki Sanari ◽  
Fumiya Sekiguchi ◽  
Ryota Sato ◽  
...  

2016 ◽  
Vol 94 (3) ◽  
Author(s):  
Xi Liu ◽  
Xiaosong Zhu ◽  
Liang Li ◽  
Yang Li ◽  
Qingbin Zhang ◽  
...  

Author(s):  
Emmanouil Skantzakis ◽  
Stefanos Chatziathanasiou ◽  
Paolo A. Carpeggiani ◽  
Giuseppe Sansone ◽  
Arjun Nayak ◽  
...  

2011 ◽  
Vol 201-203 ◽  
pp. 1590-1595
Author(s):  
Mu Zhun Zhou ◽  
Yan Ru Chen ◽  
Qi Zhao ◽  
Yu Xin

Principle of polarization encoding based on electro-optic effect of LiNbO3 crystal is analyzed, effact on polarization encoding optical field effects is studied when the incident light direction changes. Theoretical calculations show that, with the angle between the direction of incident laser beam and the main axis of LiNbO3 crystal increases, rotation angle of polarization ellipse remain unchanged,but ellipticity changes at any other position except in the center of the encoder,at the top and bottom of encoder,polarization state changes from circularly polarized to elliptically polarized,at other position of the encoder, polarization states are still elliptically polarized light but with different ellipticity angle. Experiment measurement results are in accord with ones of the calculation.


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