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PublishΝικόλας Αντωνοπούλου Modified over 6 years ago
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The Mechanism of the vdW-to-Covalent Well Transitions
We found that a small group of trajectories (~10% of the sample) make the dominant contribution to the stabilization (~65% of the cross section). They describe the super-collision events: t = a.u.
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The Mechanism of the vdW-to-Covalent Well Transitions
We found that a small group of trajectories (~10% of the sample) make the dominant contribution to the stabilization (~65% of the cross section). They describe the super-collision events: t = a.u.
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The Mechanism of the vdW-to-Covalent Well Transitions
We found that a small group of trajectories (~10% of the sample) make the dominant contribution to the stabilization (~65% of the cross section). They describe the super-collision events: t = a.u.
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The Mechanism of the vdW-to-Covalent Well Transitions
We found that a small group of trajectories (~10% of the sample) make the dominant contribution to the stabilization (~65% of the cross section). They describe the super-collision events: t = a.u.
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The Mechanism of the vdW-to-Covalent Well Transitions
We found that a small group of trajectories (~10% of the sample) make the dominant contribution to the stabilization (~65% of the cross section). They describe the super-collision events: t = a.u.
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The Mechanism of the vdW-to-Covalent Well Transitions
We found that a small group of trajectories (~10% of the sample) make the dominant contribution to the stabilization (~65% of the cross section). They describe the super-collision events: t = a.u.
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The Mechanism of the vdW-to-Covalent Well Transitions
We found that a small group of trajectories (~10% of the sample) make the dominant contribution to the stabilization (~65% of the cross section). They describe the super-collision events: t = a.u.
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The Mechanism of the vdW-to-Covalent Well Transitions
We found that a small group of trajectories (~10% of the sample) make the dominant contribution to the stabilization (~65% of the cross section). They describe the super-collision events: t = a.u.
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The Mechanism of the vdW-to-Covalent Well Transitions
We found that a small group of trajectories (~10% of the sample) make the dominant contribution to the stabilization (~65% of the cross section). They describe the super-collision events: t = a.u.
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The Mechanism of the vdW-to-Covalent Well Transitions
We found that a small group of trajectories (~10% of the sample) make the dominant contribution to the stabilization (~65% of the cross section). They describe the super-collision events: t = a.u.
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The Mechanism of the vdW-to-Covalent Well Transitions
We found that a small group of trajectories (~10% of the sample) make the dominant contribution to the stabilization (~65% of the cross section). They describe the super-collision events: t = a.u.
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The Mechanism of the vdW-to-Covalent Well Transitions
We found that a small group of trajectories (~10% of the sample) make the dominant contribution to the stabilization (~65% of the cross section). They describe the super-collision events: t = a.u.
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The Mechanism of the vdW-to-Covalent Well Transitions
We found that a small group of trajectories (~10% of the sample) make the dominant contribution to the stabilization (~65% of the cross section). They describe the super-collision events: t = a.u.
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The Mechanism of the vdW-to-Covalent Well Transitions
We found that a small group of trajectories (~10% of the sample) make the dominant contribution to the stabilization (~65% of the cross section). They describe the super-collision events: t = a.u.
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The Mechanism of the vdW-to-Covalent Well Transitions
We found that a small group of trajectories (~10% of the sample) make the dominant contribution to the stabilization (~65% of the cross section). They describe the super-collision events: t = a.u.
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The Mechanism of the vdW-to-Covalent Well Transitions
We found that a small group of trajectories (~10% of the sample) make the dominant contribution to the stabilization (~65% of the cross section). They describe the super-collision events: t = a.u.
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The Mechanism of the vdW-to-Covalent Well Transitions
We found that a small group of trajectories (~10% of the sample) make the dominant contribution to the stabilization (~65% of the cross section). They describe the super-collision events: t = a.u.
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The Mechanism of the vdW-to-Covalent Well Transitions
We found that a small group of trajectories (~10% of the sample) make the dominant contribution to the stabilization (~65% of the cross section). They describe the super-collision events: t = a.u.
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The Mechanism of the vdW-to-Covalent Well Transitions
We found that a small group of trajectories (~10% of the sample) make the dominant contribution to the stabilization (~65% of the cross section). They describe the super-collision events: t = a.u.
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The Mechanism of the vdW-to-Covalent Well Transitions
We found that a small group of trajectories (~10% of the sample) make the dominant contribution to the stabilization (~65% of the cross section). They describe the super-collision events: t = a.u.
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The Mechanism of the vdW-to-Covalent Well Transitions
We found that a small group of trajectories (~10% of the sample) make the dominant contribution to the stabilization (~65% of the cross section). They describe the super-collision events: t = a.u.
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The Mechanism of the vdW-to-Covalent Well Transitions
We found that a small group of trajectories (~10% of the sample) make the dominant contribution to the stabilization (~65% of the cross section). They describe the super-collision events: t = a.u.
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The Mechanism of the vdW-to-Covalent Well Transitions
We found that a small group of trajectories (~10% of the sample) make the dominant contribution to the stabilization (~65% of the cross section). They describe the super-collision events: t = a.u.
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The Mechanism of the vdW-to-Covalent Well Transitions
We found that a small group of trajectories (~10% of the sample) make the dominant contribution to the stabilization (~65% of the cross section). They describe the super-collision events: t = a.u.
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The Mechanism of the vdW-to-Covalent Well Transitions
We found that a small group of trajectories (~10% of the sample) make the dominant contribution to the stabilization (~65% of the cross section). They describe the super-collision events: t = a.u.
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The Mechanism of the vdW-to-Covalent Well Transitions
We found that a small group of trajectories (~10% of the sample) make the dominant contribution to the stabilization (~65% of the cross section). They describe the super-collision events: t = a.u.
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The Mechanism of the vdW-to-Covalent Well Transitions
We found that a small group of trajectories (~10% of the sample) make the dominant contribution to the stabilization (~65% of the cross section). They describe the super-collision events: t = a.u.
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The Mechanism of the vdW-to-Covalent Well Transitions
We found that a small group of trajectories (~10% of the sample) make the dominant contribution to the stabilization (~65% of the cross section). They describe the super-collision events: t = a.u.
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The Mechanism of the vdW-to-Covalent Well Transitions
We found that a small group of trajectories (~10% of the sample) make the dominant contribution to the stabilization (~65% of the cross section). They describe the super-collision events: t = a.u.
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The Mechanism of the vdW-to-Covalent Well Transitions
We found that a small group of trajectories (~10% of the sample) make the dominant contribution to the stabilization (~65% of the cross section). They describe the super-collision events: t = a.u.
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The Mechanism of the vdW-to-Covalent Well Transitions
We found that a small group of trajectories (~10% of the sample) make the dominant contribution to the stabilization (~65% of the cross section). They describe the super-collision events: t = a.u.
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The Mechanism of the vdW-to-Covalent Well Transitions
We found that a small group of trajectories (~10% of the sample) make the dominant contribution to the stabilization (~65% of the cross section). They describe the super-collision events: t = a.u.
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