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Predictive simulations of ionization energies of solvated halide ions with relativistic embedded Equation of Motion Coupled-Cluster Theory: Figures
Predictive simulations of ionization energies of solvated halide ions with relativistic embedded Equation of Motion Coupled-Cluster Theory: Figures
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Predictive simulations of ionization energies of solvated halide ions with relativistic embedded Equation of Motion Coupled-Cluster Theory: Figures

Bouchafra, Yassine ; Shee, Avijit ; Real, Florent ; Vallet, Valerie ; Gomes, Andre Severo Pereira

Zenodo 2018

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2
PIC-3
PIC-3
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PIC-3

xin, mai

figshare 2022

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3
Laser-induced symmetry breaking in energy absorption of silicon induced by ultrafast laser pulse irradiation
Laser-induced symmetry breaking in energy absorption of silicon induced by ultrafast laser pulse irradiation
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Laser-induced symmetry breaking in energy absorption of silicon induced by ultrafast laser pulse irradiation

Derrien, Thibault

figshare 2023

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4
Direct access model schematic
Direct access model schematic
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Direct access model schematic

Shravan Vasishth

figshare 2019

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5
Stainless steel spot weld defect
Stainless steel spot weld defect
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Stainless steel spot weld defect

Al Mukhtar, A.

figshare 2022

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6
Fig. 7. (a) XPS spectra monitoring the valence states of Li, Na, and K. (b) The formation energies Δ E of five different cationic lattice sites and interstitial vacancies occupied by Li in the crystal were calculated by DFT theory. (c) Positron annihilation lifetime spectra to determine the defect concentrations. (d) XPS energy spectra. (e) The ratio of Ce3+ ions to the total Ce ions in TCP:Ce, CLP:Ce, CNP:Ce, and CKP:Ce according to the XPS results. (f) The schematic diagram for the improveme
Fig. 7. (a) XPS spectra monitoring the valence states of Li, Na, and K. (b) The formation energies Δ E of five different cationic lattice sites and interstitial vacancies occupied by Li in the crystal were calculated by DFT theory. (c) Positron annihilation lifetime spectra to determine the defect concentrations. (d) XPS energy spectra. (e) The ratio of Ce3+ ions to the total Ce ions in TCP:Ce, CLP:Ce, CNP:Ce, and CKP:Ce according to the XPS results. (f) The schematic diagram for the improveme
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Fig. 7. (a) XPS spectra monitoring the valence states of Li, Na, and K. (b) The formation energies Δ E of five different cationic lattice sites and interstitial vacancies occupied by Li in the crystal were calculated by DFT theory. (c) Positron annihilation lifetime spectra to determine the defect concentrations. (d) XPS energy spectra. (e) The ratio of Ce3+ ions to the total Ce ions in TCP:Ce, CLP:Ce, CNP:Ce, and CKP:Ce according to the XPS results. (f) The schematic diagram for the improveme

Pan, Xin

figshare 2022

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Fig. 6. (a) PL spectra of TCP:Ce, TCP:Ce,Li, TCP:Ce,Na and TCP:Ce,K under 310 nm excitation. (b) PL intensity as a function of temperature (from 25 to 225 ◦C) in four samples. (c) CL spectra of TCP:Ce,Na under 10–100 mA and 8 kV. The inset shows the CL intensity of TCP:Ce and TCP:Ce,Na as a function of applied current. (d) CL spectra of TCP:Ce,Na under 60 mA and 5–15 kV. The inset shows the CL intensity of TCP:Ce and TCP:Ce,Na as a function of accelerating voltage. (e) IQE of TCP: Ce,Li, TCP
Fig. 6. (a) PL spectra of TCP:Ce, TCP:Ce,Li, TCP:Ce,Na and TCP:Ce,K under 310 nm excitation. (b) PL intensity as a function of temperature (from 25 to 225 ◦C) in four samples. (c) CL spectra of TCP:Ce,Na under 10–100 mA and 8 kV. The inset shows the CL intensity of TCP:Ce and TCP:Ce,Na as a function of applied current. (d) CL spectra of TCP:Ce,Na under 60 mA and 5–15 kV. The inset shows the CL intensity of TCP:Ce and TCP:Ce,Na as a function of accelerating voltage. (e) IQE of TCP: Ce,Li, TCP
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Fig. 6. (a) PL spectra of TCP:Ce, TCP:Ce,Li, TCP:Ce,Na and TCP:Ce,K under 310 nm excitation. (b) PL intensity as a function of temperature (from 25 to 225 ◦C) in four samples. (c) CL spectra of TCP:Ce,Na under 10–100 mA and 8 kV. The inset shows the CL intensity of TCP:Ce and TCP:Ce,Na as a function of applied current. (d) CL spectra of TCP:Ce,Na under 60 mA and 5–15 kV. The inset shows the CL intensity of TCP:Ce and TCP:Ce,Na as a function of accelerating voltage. (e) IQE of TCP: Ce,Li, TCP

Pan, Xin

figshare 2022

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8
Local Sequence Alignment Experiment (70)
Local Sequence Alignment Experiment (70)
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Local Sequence Alignment Experiment (70)

Gagniuc, Paul A.

figshare 2022

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9
Creating a Prototype Atmospheric Dispersion Digital Twin: Lowering barrier to data access and production
Creating a Prototype Atmospheric Dispersion Digital Twin: Lowering barrier to data access and production
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Creating a Prototype Atmospheric Dispersion Digital Twin: Lowering barrier to data access and production

Haddad, Stephen

ESIP 2022

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Infographic for pivot_wider()
Infographic for pivot_wider()
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Infographic for pivot_wider()

Rajeg, Gede Primahadi Wijaya

figshare 2020

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  • Realização: ABCD-USP USP   Logos de Redes Sociais: Freepik

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