1
|
Riffe EJ, Bernal F, Kamal C, Mizuno H, Lindsey RK, Hamel S, Raj SL, Hull CJ, Kwon S, Park SH, Cooper JK, Yang F, Liu YS, Guo J, Nordlund D, Drisdell WS, Zuerch MW, Whitley HD, Odelius M, Schwartz CP, J Saykally R. Time-Resolved X-ray Emission Spectroscopy and Resonant Inelastic X-ray Scattering Spectroscopy of Laser Irradiated Carbon. J Phys Chem B 2024; 128:6422-6433. [PMID: 38906826 DOI: 10.1021/acs.jpcb.4c02862] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Indexed: 06/23/2024]
Abstract
The existence of liquid carbon as an intermediate phase preceding the formation of novel carbon materials has been a point of contention for several decades. Experimental observation of such a liquid state requires nonthermal melting of solid carbon materials at various laser fluences and pulse properties. Reflectivity experiments performed in the mid-1980s reached opposing conclusions regarding the metallic or insulating properties of the purported liquid state. Time-resolved X-ray absorption studies showed shortening of C-C bonds and increasing diffraction densities, thought to evidence a liquid or glassy carbon state, respectively. Nevertheless, none of these experiments provided information on the electronic structure of the proposed liquid state. Herein, we report the results of time-resolved resonant inelastic X-ray scattering (RIXS) and time-resolved X-ray emission spectroscopy (XES) studies on amorphous carbon (a-C) and ultrananocrystalline diamond (UNCD) as a function of delay time between the irradiating pulse and X-ray probe. For both a-C and UNCD, we attribute decreases in RIXS or XES signals to transition blocking, relaxation, and finally, ablation. Increased signal at 20 ps following the irradiation of the UNCD is attributed to the probable formation of nanoscale structures in the ablation plume. Differences in the amount of signal observed between a-C and UNCD are explained by the difference in sample thickness and, specifically, incomplete melting of the UNCD film. Comparisons to spectral simulations based on MD trajectories at extreme conditions indicate that the carbon state in our experiments is crystalline. Normal mode analysis confirmed that symmetrical bending or stretching of the C-C bonds in the diamond lattice results in XES spectra with small intensity differences. Overall, we observed no evidence of melting to a liquid state, as determined by the lack of changes in the spectral properties for up to 100 ps delays following the melting pulses.
Collapse
Affiliation(s)
- Erika J Riffe
- Department of Chemistry, University of California, Berkeley, Berkeley, California 94720, United States
| | - Franky Bernal
- Department of Chemistry, University of California, Berkeley, Berkeley, California 94720, United States
- Chemical Sciences Division, Lawrence Berkeley National Laboratory, Berkeley, California 94720, United States
| | - Chinnathambi Kamal
- Theory and Simulations Laboratory, Theoretical and Computational Physics Section, Raja Ramanna Centre for Advanced Technology, Indore 452013, India
- Homi Bhabha National Institute, Training School Complex, Anushakti Nagar, Mumbai, Maharashtra 400094, India
| | - Hikaru Mizuno
- Department of Chemistry, University of California, Berkeley, Berkeley, California 94720, United States
- Chemical Sciences Division, Lawrence Berkeley National Laboratory, Berkeley, California 94720, United States
| | - Rebecca K Lindsey
- Lawrence Livermore National Laboratory, 7000 East Avenue, Livermore, California 94550, United States
- Department of Chemical Engineering, University of Michigan, Ann Arbor, Michigan 48109, United States
| | - Sebastien Hamel
- Lawrence Livermore National Laboratory, 7000 East Avenue, Livermore, California 94550, United States
| | - Sumana L Raj
- Department of Chemistry, University of California, Berkeley, Berkeley, California 94720, United States
- Chemical Sciences Division, Lawrence Berkeley National Laboratory, Berkeley, California 94720, United States
| | - Christopher J Hull
- Department of Chemistry, University of California, Berkeley, Berkeley, California 94720, United States
- Chemical Sciences Division, Lawrence Berkeley National Laboratory, Berkeley, California 94720, United States
| | - Soonnam Kwon
- PAL-XFEL, Pohang Accelerator Laboratory, 77 Cheongam-Ro, Nam-Gu, Pohang, Gyeongbuk 37673, South Korea
| | - Sang Han Park
- PAL-XFEL, Pohang Accelerator Laboratory, 77 Cheongam-Ro, Nam-Gu, Pohang, Gyeongbuk 37673, South Korea
| | - Jason K Cooper
- Chemical Sciences Division, Lawrence Berkeley National Laboratory, Berkeley, California 94720, United States
- Liquid Sunlight Alliance, Lawrence Berkeley National Laboratory, Berkeley, California 94720, United States
| | - Feipeng Yang
- Advanced Light Source, Lawrence Berkeley National Laboratory, Berkeley, California 94720, United States
| | - Yi-Sheng Liu
- Advanced Light Source, Lawrence Berkeley National Laboratory, Berkeley, California 94720, United States
| | - Jinghua Guo
- Advanced Light Source, Lawrence Berkeley National Laboratory, Berkeley, California 94720, United States
| | - Dennis Nordlund
- Stanford Synchrotron Radiation Lightsource, SLAC National Accelerator Laboratory, Menlo Park, California 94025, United States
| | - Walter S Drisdell
- Chemical Sciences Division, Lawrence Berkeley National Laboratory, Berkeley, California 94720, United States
- Liquid Sunlight Alliance, Lawrence Berkeley National Laboratory, Berkeley, California 94720, United States
| | - Michael W Zuerch
- Department of Chemistry, University of California, Berkeley, Berkeley, California 94720, United States
- Materials Science Division, Lawerence Berkeley National Laboratory, Berkeley, California 94720, United States
| | - Heather D Whitley
- Lawrence Livermore National Laboratory, 7000 East Avenue, Livermore, California 94550, United States
| | - Michael Odelius
- Department of Physics, Stockholm University, 10691 Stockholm, Sweden
| | - Craig P Schwartz
- Chemical Sciences Division, Lawrence Berkeley National Laboratory, Berkeley, California 94720, United States
- Nevada Extreme Conditions Laboratory, University of Nevada, Las Vegas, Las Vegas, Nevada 89154, United States
| | - Richard J Saykally
- Department of Chemistry, University of California, Berkeley, Berkeley, California 94720, United States
- Chemical Sciences Division, Lawrence Berkeley National Laboratory, Berkeley, California 94720, United States
| |
Collapse
|
3
|
Wang X, Jarnac A, Ekström JC, Bengtsson ÅUJ, Dorchies F, Enquist H, Jurgilaitis A, Pedersen MN, Tu CM, Wulff M, Larsson J. Generation of a large compressive strain wave in graphite by ultrashort-pulse laser irradiation. STRUCTURAL DYNAMICS (MELVILLE, N.Y.) 2019; 6:024501. [PMID: 30915389 PMCID: PMC6422787 DOI: 10.1063/1.5089291] [Citation(s) in RCA: 1] [Impact Index Per Article: 0.2] [Reference Citation Analysis] [Abstract] [Track Full Text] [Figures] [Subscribe] [Scholar Register] [Received: 01/18/2019] [Accepted: 03/04/2019] [Indexed: 06/09/2023]
Abstract
We have studied strain wave generation in graphite induced by an intense ultrashort laser pulse. The study was performed in the intensity regime above the ablation threshold of graphite. The aim was to maximize the strain and, thus, also the internal pressure (stress). Laser pulses with a 1 ps temporal duration melt the surface of graphite resulting in a molten material which initially exists at the solid density. As the molten material expands, a compressive strain wave starts propagating into the crystal below the molten layer. The strain pulse was studied with time-resolved X-ray diffraction. At a temporal delay of 100 ps after laser excitation, we observed >10% compressive strain, which corresponds to a pressure of 7.2 GPa. This strain could be reproduced by hydrodynamic simulations, which also provided a temperature map as a function of time and depth.
Collapse
Affiliation(s)
- Xiaocui Wang
- Department of Physics, Lund University, P.O. Box 118, SE-221 00 Lund, Sweden
| | | | - J. C. Ekström
- Department of Physics, Lund University, P.O. Box 118, SE-221 00 Lund, Sweden
| | - Å. U. J. Bengtsson
- Department of Physics, Lund University, P.O. Box 118, SE-221 00 Lund, Sweden
| | - F. Dorchies
- Université de Bordeaux, CNRS, CEA, CELIA (Centre Lasers Intenses et Applications), UMR 5107, F-33400 Talence, France
| | - H. Enquist
- MAX IV Laboratory, Lund University, P.O. Box 118, SE-221 00 Lund, Sweden
| | - A. Jurgilaitis
- MAX IV Laboratory, Lund University, P.O. Box 118, SE-221 00 Lund, Sweden
| | - M. N. Pedersen
- ESRF-The European Synchrotron, CS40220, 38043 Grenoble Cedex 9, France
| | - C.-M. Tu
- Department of Physics, Lund University, P.O. Box 118, SE-221 00 Lund, Sweden
| | - M. Wulff
- ESRF-The European Synchrotron, CS40220, 38043 Grenoble Cedex 9, France
| | - J. Larsson
- Author to whom correspondence should be addressed:
| |
Collapse
|