Details of the experiment
We use the same apparatus that we used in our previous work20 to perform laser spectroscopy of an E2 transition in \({{\rm{H}}}_{2}^{+}\) and HD+. We prepare a cluster of trapped and sympathetically cooled molecular ions,…
We use the same apparatus that we used in our previous work20 to perform laser spectroscopy of an E2 transition in \({{\rm{H}}}_{2}^{+}\) and HD+. We prepare a cluster of trapped and sympathetically cooled molecular ions,…
The crystal structure of the M2B2H4 monolayer is illustrated in Fig. 1. Layered M2B2H4 adopts a 3D hexagonal structure with a space group symmetry of P6/mmm, analogous to Mg2B2. Figure 1 presents the side view and top view of…
Given a QNN \(\hat{U}({\boldsymbol{\theta }})\) with L variational parameters θ = (θ1, …, θL), we consider a supervised learning task involving N quantum data \({\{\vert {\psi }_{\alpha }\rangle \}}_{\alpha = 1}^{N}\),…
At a time of growing catastrophic risks posed by climate change, pandemics and advances in artificial intelligence (AI), and more than 30 years after the end of the cold war, many people consider nuclear weapons to be relics of the twentieth…
The first chemical reactions in the wake of the Big Bang have been recreated for the first time in conditions similar to those in the baby Universe.
A team of physicists Led by Florian Grussie of the Max Planck Institute for Nuclear Physics…
• Physics 18, s108
A new experimental design eliminates the top source of clock uncertainty.
Optical lattice clocks (OLCs) are among the world’s best atomic clocks. Their largest source of uncertainty results from the…
Kjaergaard, M. et al. Superconducting qubits: current state of play. Annu. Rev. Condens. Matter Phys. 11, 369 (2020).
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Likharev, K. K. Superconducting weak links. Rev. Mod. Phys. 51,…
This section describes the methods used to estimate the type and location of the first point of interaction of 511 keV gamma photons in monolithic scintillator blocks. The methodology involves three main steps:
Figure 1 a illustrates the 3D microwave cavities used in our system, each with four ports featuring adjustable coupling rates, tunable (identical) resonance frequency, ωc, and fixed internal loss rates, κint. Figure 1b presents an exploded…
The structure after relaxation has a lattice constant equal to 14.3185 Å for B1 and 14.3004 Å for T1. This value is almost 5% greater than the experimentally determined value 13.6740 . With the GGA, the overestimation of…