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13141
In Situ Mechanochemical Modulation of Carbon Nanotube Forest Growth
Published 2018“…By correlating in situ kinetics measurements with spatial mapping of CNT orientation and density by X-ray scattering, we find that the average growth rate of individual CNTs is also mechanically modulated; specifically, a 100-fold increase in force causes a 4-fold decrease in average CNT lengthening rate. …”
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13142
In Situ Mechanochemical Modulation of Carbon Nanotube Forest Growth
Published 2018“…By correlating in situ kinetics measurements with spatial mapping of CNT orientation and density by X-ray scattering, we find that the average growth rate of individual CNTs is also mechanically modulated; specifically, a 100-fold increase in force causes a 4-fold decrease in average CNT lengthening rate. …”
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13143
Molecular Structures, Dipole Moments, and Electronic Properties of β‑HMX under External Electric Field from First-Principles Calculations
Published 2024“…When the external electric field is increasing along the [100], [010], and [001] crystallographic directions of β-HMX, the calculation results indicate that an increase in the bond length (N1–N3/N1′–N3′) of the triggering bond, an increase in the main <i>Q</i><sub>nitro</sub> (N3, N3′) value, an increase in the minimum surface electrostatic potential, and a decrease in band gap all contribute to a reduction in its stability. …”
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13144
Molecular Structures, Dipole Moments, and Electronic Properties of β‑HMX under External Electric Field from First-Principles Calculations
Published 2024“…When the external electric field is increasing along the [100], [010], and [001] crystallographic directions of β-HMX, the calculation results indicate that an increase in the bond length (N1–N3/N1′–N3′) of the triggering bond, an increase in the main <i>Q</i><sub>nitro</sub> (N3, N3′) value, an increase in the minimum surface electrostatic potential, and a decrease in band gap all contribute to a reduction in its stability. …”
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13145
Molecular Structures, Dipole Moments, and Electronic Properties of β‑HMX under External Electric Field from First-Principles Calculations
Published 2024“…When the external electric field is increasing along the [100], [010], and [001] crystallographic directions of β-HMX, the calculation results indicate that an increase in the bond length (N1–N3/N1′–N3′) of the triggering bond, an increase in the main <i>Q</i><sub>nitro</sub> (N3, N3′) value, an increase in the minimum surface electrostatic potential, and a decrease in band gap all contribute to a reduction in its stability. …”
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13146
Molecular Structures, Dipole Moments, and Electronic Properties of β‑HMX under External Electric Field from First-Principles Calculations
Published 2024“…When the external electric field is increasing along the [100], [010], and [001] crystallographic directions of β-HMX, the calculation results indicate that an increase in the bond length (N1–N3/N1′–N3′) of the triggering bond, an increase in the main <i>Q</i><sub>nitro</sub> (N3, N3′) value, an increase in the minimum surface electrostatic potential, and a decrease in band gap all contribute to a reduction in its stability. …”
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13147
Molecular Structures, Dipole Moments, and Electronic Properties of β‑HMX under External Electric Field from First-Principles Calculations
Published 2024“…When the external electric field is increasing along the [100], [010], and [001] crystallographic directions of β-HMX, the calculation results indicate that an increase in the bond length (N1–N3/N1′–N3′) of the triggering bond, an increase in the main <i>Q</i><sub>nitro</sub> (N3, N3′) value, an increase in the minimum surface electrostatic potential, and a decrease in band gap all contribute to a reduction in its stability. …”
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13148
Molecular Structures, Dipole Moments, and Electronic Properties of β‑HMX under External Electric Field from First-Principles Calculations
Published 2024“…When the external electric field is increasing along the [100], [010], and [001] crystallographic directions of β-HMX, the calculation results indicate that an increase in the bond length (N1–N3/N1′–N3′) of the triggering bond, an increase in the main <i>Q</i><sub>nitro</sub> (N3, N3′) value, an increase in the minimum surface electrostatic potential, and a decrease in band gap all contribute to a reduction in its stability. …”
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13149
Molecular Structures, Dipole Moments, and Electronic Properties of β‑HMX under External Electric Field from First-Principles Calculations
Published 2024“…When the external electric field is increasing along the [100], [010], and [001] crystallographic directions of β-HMX, the calculation results indicate that an increase in the bond length (N1–N3/N1′–N3′) of the triggering bond, an increase in the main <i>Q</i><sub>nitro</sub> (N3, N3′) value, an increase in the minimum surface electrostatic potential, and a decrease in band gap all contribute to a reduction in its stability. …”
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13150
Molecular Structures, Dipole Moments, and Electronic Properties of β‑HMX under External Electric Field from First-Principles Calculations
Published 2024“…When the external electric field is increasing along the [100], [010], and [001] crystallographic directions of β-HMX, the calculation results indicate that an increase in the bond length (N1–N3/N1′–N3′) of the triggering bond, an increase in the main <i>Q</i><sub>nitro</sub> (N3, N3′) value, an increase in the minimum surface electrostatic potential, and a decrease in band gap all contribute to a reduction in its stability. …”
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13151
Molecular Structures, Dipole Moments, and Electronic Properties of β‑HMX under External Electric Field from First-Principles Calculations
Published 2024“…When the external electric field is increasing along the [100], [010], and [001] crystallographic directions of β-HMX, the calculation results indicate that an increase in the bond length (N1–N3/N1′–N3′) of the triggering bond, an increase in the main <i>Q</i><sub>nitro</sub> (N3, N3′) value, an increase in the minimum surface electrostatic potential, and a decrease in band gap all contribute to a reduction in its stability. …”
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13152
Molecular Structures, Dipole Moments, and Electronic Properties of β‑HMX under External Electric Field from First-Principles Calculations
Published 2024“…When the external electric field is increasing along the [100], [010], and [001] crystallographic directions of β-HMX, the calculation results indicate that an increase in the bond length (N1–N3/N1′–N3′) of the triggering bond, an increase in the main <i>Q</i><sub>nitro</sub> (N3, N3′) value, an increase in the minimum surface electrostatic potential, and a decrease in band gap all contribute to a reduction in its stability. …”
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13153
Molecular Structures, Dipole Moments, and Electronic Properties of β‑HMX under External Electric Field from First-Principles Calculations
Published 2024“…When the external electric field is increasing along the [100], [010], and [001] crystallographic directions of β-HMX, the calculation results indicate that an increase in the bond length (N1–N3/N1′–N3′) of the triggering bond, an increase in the main <i>Q</i><sub>nitro</sub> (N3, N3′) value, an increase in the minimum surface electrostatic potential, and a decrease in band gap all contribute to a reduction in its stability. …”
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13154
Molecular Structures, Dipole Moments, and Electronic Properties of β‑HMX under External Electric Field from First-Principles Calculations
Published 2024“…When the external electric field is increasing along the [100], [010], and [001] crystallographic directions of β-HMX, the calculation results indicate that an increase in the bond length (N1–N3/N1′–N3′) of the triggering bond, an increase in the main <i>Q</i><sub>nitro</sub> (N3, N3′) value, an increase in the minimum surface electrostatic potential, and a decrease in band gap all contribute to a reduction in its stability. …”
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13155
Molecular Structures, Dipole Moments, and Electronic Properties of β‑HMX under External Electric Field from First-Principles Calculations
Published 2024“…When the external electric field is increasing along the [100], [010], and [001] crystallographic directions of β-HMX, the calculation results indicate that an increase in the bond length (N1–N3/N1′–N3′) of the triggering bond, an increase in the main <i>Q</i><sub>nitro</sub> (N3, N3′) value, an increase in the minimum surface electrostatic potential, and a decrease in band gap all contribute to a reduction in its stability. …”
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13156
Molecular Structures, Dipole Moments, and Electronic Properties of β‑HMX under External Electric Field from First-Principles Calculations
Published 2024“…When the external electric field is increasing along the [100], [010], and [001] crystallographic directions of β-HMX, the calculation results indicate that an increase in the bond length (N1–N3/N1′–N3′) of the triggering bond, an increase in the main <i>Q</i><sub>nitro</sub> (N3, N3′) value, an increase in the minimum surface electrostatic potential, and a decrease in band gap all contribute to a reduction in its stability. …”
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13157
Molecular Structures, Dipole Moments, and Electronic Properties of β‑HMX under External Electric Field from First-Principles Calculations
Published 2024“…When the external electric field is increasing along the [100], [010], and [001] crystallographic directions of β-HMX, the calculation results indicate that an increase in the bond length (N1–N3/N1′–N3′) of the triggering bond, an increase in the main <i>Q</i><sub>nitro</sub> (N3, N3′) value, an increase in the minimum surface electrostatic potential, and a decrease in band gap all contribute to a reduction in its stability. …”
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13158
Molecular Structures, Dipole Moments, and Electronic Properties of β‑HMX under External Electric Field from First-Principles Calculations
Published 2024“…When the external electric field is increasing along the [100], [010], and [001] crystallographic directions of β-HMX, the calculation results indicate that an increase in the bond length (N1–N3/N1′–N3′) of the triggering bond, an increase in the main <i>Q</i><sub>nitro</sub> (N3, N3′) value, an increase in the minimum surface electrostatic potential, and a decrease in band gap all contribute to a reduction in its stability. …”
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13159
Molecular Structures, Dipole Moments, and Electronic Properties of β‑HMX under External Electric Field from First-Principles Calculations
Published 2024“…When the external electric field is increasing along the [100], [010], and [001] crystallographic directions of β-HMX, the calculation results indicate that an increase in the bond length (N1–N3/N1′–N3′) of the triggering bond, an increase in the main <i>Q</i><sub>nitro</sub> (N3, N3′) value, an increase in the minimum surface electrostatic potential, and a decrease in band gap all contribute to a reduction in its stability. …”
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13160
Molecular Structures, Dipole Moments, and Electronic Properties of β‑HMX under External Electric Field from First-Principles Calculations
Published 2024“…When the external electric field is increasing along the [100], [010], and [001] crystallographic directions of β-HMX, the calculation results indicate that an increase in the bond length (N1–N3/N1′–N3′) of the triggering bond, an increase in the main <i>Q</i><sub>nitro</sub> (N3, N3′) value, an increase in the minimum surface electrostatic potential, and a decrease in band gap all contribute to a reduction in its stability. …”