Rydberg state excitation in molecules manipulated by bicircular two-color laser pulses

Wenbin Zhang; Yongzhe Ma; Chenxu Lu; Fei Chen; Shengzhe Pan; Peifen Lu; Hongcheng Ni; Jian Wu

doi:10.1117/1.AP.5.1.016002

Journals >Advanced Photonics >Volume 5 >Issue 1 >Page 016002 > Article

Advanced Photonics
Vol. 5, Issue 1, 016002 (2023)

Rydberg state excitation in molecules manipulated by bicircular two-color laser pulses

Wenbin Zhang^{1、2、3、*}, Yongzhe Ma¹, Chenxu Lu¹, Fei Chen¹, Shengzhe Pan¹, Peifen Lu¹, Hongcheng Ni^1、4、*, and Jian Wu^{1、4、5、*}

Author Affiliations

¹East China Normal University, State Key Laboratory of Precision Spectroscopy, Shanghai, China

²Ludwig-Maximilians-Universität Munich, Department of Physics, Garching, Germany

³Max Planck Institute of Quantum Optics, Garching, Germany

⁴Shanxi University, Collaborative Innovation Center of Extreme Optics, Taiyuan, China

⁵CAS Center for Excellence in Ultra-Intense Laser Science, Shanghai, China

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DOI: 10.1117/1.AP.5.1.016002 Cite this Article

Wenbin Zhang, Yongzhe Ma, Chenxu Lu, Fei Chen, Shengzhe Pan, Peifen Lu, Hongcheng Ni, Jian Wu. Rydberg state excitation in molecules manipulated by bicircular two-color laser pulses[J]. Advanced Photonics, 2023, 5(1): 016002 Copy Citation Text

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Experimental scheme. (a) Schematic illustration of the experimental setup to study the RSE of the H2 molecules with BCTC laser fields. (b), (c) Measured (b) PEPICO and (c) PIPICO spectrum of the H2 molecule. The H2+ signals created from the postpulse ionization of H2* and from the strong-field ionization H2 can be distinguished in the PEPICO spectrum, while the (H+,H*) and (H+,H+) channels can be unambiguously identified in the PIPICO spectrum. (d), (e) Combined electric fields Ey versus Ez as well as the corresponding vector potential Ay versus Az for the (d) counterrotating and (e) co-rotating circularly polarized two-color laser fields with a field ratio of ESH/EFW=1.5.

Fig. 1. Experimental scheme. (a) Schematic illustration of the experimental setup to study the RSE of the

H_{2}

molecules with BCTC laser fields. (b), (c) Measured (b) PEPICO and (c) PIPICO spectrum of the

H_{2}

molecule. The

H_{2}^{+}

signals created from the postpulse ionization of

{H_{2}}^{*}

and from the strong-field ionization

H_{2}

can be distinguished in the PEPICO spectrum, while the

(H^{+}, H^{*})

and

(H^{+}, H^{+})

channels can be unambiguously identified in the PIPICO spectrum. (d), (e) Combined electric fields

E_{y}

versus

E_{z}

as well as the corresponding vector potential

A_{y}

versus

A_{z}

for the (d) counterrotating and (e) co-rotating circularly polarized two-color laser fields with a field ratio of

E_{SH} / E_{FW} = 1.5

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Manipulation of RSE yield by BCTC laser pulses. (a) Experimentally measured yields of the Rydberg fragments of H2* and (H+,H*) channels created in the interaction of the H2 molecules with BCTC laser fields. Solid and open symbols represent the counterrotating and co-rotating cases, respectively. The thick arrows near the right ordinate indicate the measured yield of the H2* and (H+,H*) channels employing a single-color SH circularly polarized laser pulse. The yield of each data point is normalized to a single laser shot. (b) The corresponding yield ratios between the counterrotating and co-rotating cases of the RSE channels displayed in panel (a). The shapes of combined electric fields of the BCTC fields for different field ratios and polarization helicities are illustrated in the inset of panel (b). (c) Numerically simulated Rydberg yields of H* for the counterrotating and co-rotating cases of the BCTC laser pulse. The yield of each data point is normalized to the simulated total number of released electrons. The right ordinate shows the inverse of the magnitude of the vector potential [−A(t)] of the counterrotating and co-rotating fields where the field amplitude maximizes. The case without the photon effect is shown in blue, and the other case with the photon effect included is shown in orange. (d) The corresponding yield ratios between the counterrotating and co-rotating cases of the simulated Rydberg yield of H* for the two cases in panel (c).

Fig. 2. Manipulation of RSE yield by BCTC laser pulses. (a) Experimentally measured yields of the Rydberg fragments of

{H_{2}}^{*}

and

(H^{+}, H^{*})

channels created in the interaction of the

H_{2}

molecules with BCTC laser fields. Solid and open symbols represent the counterrotating and co-rotating cases, respectively. The thick arrows near the right ordinate indicate the measured yield of the

{H_{2}}^{*}

and

(H^{+}, H^{*})

channels employing a single-color SH circularly polarized laser pulse. The yield of each data point is normalized to a single laser shot. (b) The corresponding yield ratios between the counterrotating and co-rotating cases of the RSE channels displayed in panel (a). The shapes of combined electric fields of the BCTC fields for different field ratios and polarization helicities are illustrated in the inset of panel (b). (c) Numerically simulated Rydberg yields of

H^{*}

for the counterrotating and co-rotating cases of the BCTC laser pulse. The yield of each data point is normalized to the simulated total number of released electrons. The right ordinate shows the inverse of the magnitude of the vector potential

[- A (t)]

of the counterrotating and co-rotating fields where the field amplitude maximizes. The case without the photon effect is shown in blue, and the other case with the photon effect included is shown in orange. (d) The corresponding yield ratios between the counterrotating and co-rotating cases of the simulated Rydberg yield of

H^{*}

for the two cases in panel (c).

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Fig. 3. Field-ratio-resolved KER spectra of the fragmentation channels in the co-rotating case. (a), (b) Measured KER distributions of the nuclear fragments of (a) the