{"process": "Reflection", "process_types": [{"abbreviation": "MRF", "description": "Reflection"}, {"abbreviation": "MRH", "description": "Reflection of Heavy Particles from Surfaces"}], "surface": "Li2O", "surface_phase": "a", "species": {"text": "H", "charge": 0}, "temperature": 300, "comment": "", "refs": [{"id": 4, "authors": "P. S. Krstic, E. T. Ostrowski, S. Dwivedi, S. Abe, A. Maan, A. C. T. Van Duin, B. E. Koel", "title": "Detailed studies of the processes in low energy H irradiation of Li and Li-compound surfaces", "journal": "Journal of Applied Physics", "volume": "134", "page_start": "", "page_end": "", "article_number": "", "year": 2023, "note": "", "doi": "10.1063/5.0149502", "bibcode": "2023JAP...134j0902K", "url": "https://dx.doi.org/10.1063/5.0149502"}]}
------------------------------------------------------------------------
Reflection of H on Li2O(a) at 300 K
angle = 0.0 deg
E /eV	P	unc
1.0	0.1208	0.0109
5.0	0.4016	0.0202
10.0	0.3462	0.0188
25.0	0.2114	0.0155
50.0	0.1007	0.011
75.0	0.0623	0.0086
100.0	0.0373	0.0068
-----

angle = 45.0 deg
E /eV	P	unc
1.0	0.1298	0.0122
5.0	0.5444	0.0249
10.0	0.4449	0.0225
25.0	0.2731	0.0184
50.0	0.1503	0.0137
75.0	0.0808	0.0102
100.0	0.0371	0.007
-----

angle = 85.0 deg
E /eV	P	unc
1.0	0.1163	0.0126
5.0	0.6059	0.0243
10.0	0.525	0.0227
25.0	0.5676	0.0236
50.0	0.478	0.0216
75.0	0.431	0.021
100.0	0.4035	0.0199
-----

Reflection of H on Li2O(a) at 300 K
E = 1.0 eV
angle /deg	P	unc
0.0		0.1208	0.0109
45.0		0.1298	0.0122
85.0		0.1163	0.0126
-----

E = 5.0 eV
angle /deg	P	unc
0.0		0.4016	0.0202
45.0		0.5444	0.0249
85.0		0.6059	0.0243
-----

E = 10.0 eV
angle /deg	P	unc
0.0		0.3462	0.0188
45.0		0.4449	0.0225
85.0		0.525	0.0227
-----

E = 25.0 eV
angle /deg	P	unc
0.0		0.2114	0.0155
45.0		0.2731	0.0184
85.0		0.5676	0.0236
-----

E = 50.0 eV
angle /deg	P	unc
0.0		0.1007	0.011
45.0		0.1503	0.0137
85.0		0.478	0.0216
-----

E = 75.0 eV
angle /deg	P	unc
0.0		0.0623	0.0086
45.0		0.0808	0.0102
85.0		0.431	0.021
-----

E = 100.0 eV
angle /deg	P	unc
0.0		0.0373	0.0068
45.0		0.0371	0.007
85.0		0.4035	0.0199
-----