Purely Spatial Quantum Diffusion of H Atoms in Solid H_{2} at Temperatures below 1 K
S Sheludiakov1, D M Lee1, V V Khmelenko1
1Institute for Quantum Science and Engineering, Department of Physics and Astronomy, Texas A&M University, College Station, Texas 77843, USA.
Physical Review Letters
|May 28, 2021
Summary
We directly measured quantum diffusion of hydrogen (H) atoms in solid molecular hydrogen (H2) films at 0.7 K. This diffusion rate is orders of magnitude faster than previously estimated, revealing enhanced mobility with phonon injection.
Area of Science:
- Quantum physics
- Condensed matter physics
- Materials science
Background:
- Atomic diffusion in solid molecular hydrogen (H2) is poorly understood at low temperatures.
- Previous studies relied on indirect methods like H atom recombination to infer H atom mobility.
- Understanding atomic transport in solid H2 is crucial for fields like quantum computing and astrophysics.
Purpose of the Study:
- To directly measure the quantum diffusion rate of H atoms in solid H2 films at ultralow temperatures.
- To investigate the influence of phonons on H atom mobility.
- To provide a more accurate characterization of H atom transport in solid H2.
Main Methods:
- Direct measurement of H atom quantum diffusion using a novel technique.
- Experiments conducted on solid H2 films at a temperature of 0.7 K.
- Controlled injection of phonons to study their effect on diffusion.
Main Results:
- A pure spatial diffusion rate of H atoms in H2 films was determined to be D^d = 5(2)×10^-17 cm^2 s^-1.
- This measured diffusion rate is two orders of magnitude faster than previously inferred values.
- H atom diffusion was observed to be significantly enhanced by the injection of phonons.
Conclusions:
- This study presents the first direct measurement of pure spatial diffusion for H atoms in solid H2.
- The findings challenge previous assumptions about H atom mobility in solid H2.
- Solid H2, alongside helium-3/helium-4 mixtures, is confirmed as a rare system exhibiting non-vanishing atomic diffusion below 1 K.
Related Concept Videos
Hydrogen Bonds
128.1K
Hydrogen bonds are weak attractions between atoms that have formed other chemical bonds. One of these atoms is electronegative, like oxygen, and has a partial negative charge. The other is a hydrogen atom that has bonded with another electronegative atom and has a partial positive charge.
Hydrogen Bonds Control the World!
Because hydrogen has very weak electronegativity when it binds with a strongly electronegative atom, such as oxygen or nitrogen, electrons in the bond are unequally shared....
Hydrogen Bonds Control the World!
Because hydrogen has very weak electronegativity when it binds with a strongly electronegative atom, such as oxygen or nitrogen, electrons in the bond are unequally shared....
128.1K
Hydrogen Bonds
11.4K
A hydrogen bond is formed when a weakly positive hydrogen atom already bonded to one electronegative atom (for example, the oxygen in the water molecule) is attracted to another electronegative atom from another polar molecule, such as water (H2O), hydrogen fluoride (HF), or ammonia (NH3). The huge electronegativity difference between the H atom (2.1) and the atom to which it is bonded (4.0 for an F atom, 3.5 for an O atom, or 3.0 for an N atom), combined with the very small size of an H atom...
11.4K
Emission Spectra
72.6K
When solids, liquids, or condensed gases are heated sufficiently, they radiate some of the excess energy as light. Photons produced in this manner have a range of energies, and thereby produce a continuous spectrum in which an unbroken series of wavelengths is present.
72.6K
Atomic Nuclei: Nuclear Spin State Population Distribution
1.5K
Near absolute zero temperatures, in the presence of a magnetic field, the majority of nuclei prefer the lower energy spin-up state to the higher energy spin-down state. As temperatures increase, the energy from thermal collisions distributes the spins more equally between the two states. The Boltzmann distribution equation gives the ratio of the number of spins predicted in the spin −½ (N−) and spin +½ (N+) states.
1.5K
Escape Velocities of Gases
1.1K
To escape the Earth's gravity, an object near the top of the atmosphere at an altitude of 100 km must travel away from Earth at 11.1 km/s. This speed is called the escape velocity. The temperature at which gas molecules attain the rms speed, which is equal to the escape velocity, can be estimated by using the equation for the average kinetic energy of the gas molecules. According to the kinetic theory of gas, the average kinetic energy of the gas molecules is proportional to its...
1.1K
The Bohr Model
76.8K
Following the work of Ernest Rutherford and his colleagues in the early twentieth century, the picture of atoms consisting of tiny dense nuclei surrounded by lighter and even tinier electrons continually moving about the nucleus was well established. This picture was called the planetary model since it pictured the atom as a miniature “solar system” with the electrons orbiting the nucleus like planets orbiting the sun. The simplest atom is hydrogen, consisting of a single proton as the...
76.8K


