SI1: Sample characterization by HPLC and CW-EPR spectroscopy. Figure S1: (a) Anion exchange traces of purified single-stranded double-C T -labeled RNAs. (b) Spin concentration calibration curve. (c) RNA labelling efficiency. SI2: Examination of orientation selection. Figure S2: Highand low-power Q-band DEER on [13,28] RNA duplex. Figure S3: High-power Q-band DEER on different RNA samples. Figur...

I. Overview of the computation Reviewing the setup from our lecture notes of last year [S1], we let R denote a crystallographic root system with V the ambient real Euclidean space, along with the usual choices (simple roots, positive roots,...), and W the Weyl group. Given a reduced expression for the longest element of the Weyl group, say w0 = si1 · · · sil , there is an induced ordering β ∨ 1...

The changes in the electrical and physical properties of HfO2 films grown using atomic layer deposition (ALD) on Si1-XGeX (x=0.1, 0.2, 0.3) substrates after post-annealing have been studied. The migration of Ge plays a key role in reducing the capacitance equivalent thickness (CET) whilst keeping the leakage current density constant after post-annealing. The Ge atoms which have already diffused...

Si1-xGexnanocrystals (NCs) of different composition and size were generated using the Molecular Dynamics (MD) method by minimizing NC’s total energy calculated using Tersoff’s empirical potential and applying rigid boundary conditions. The dynamical matrix of the relaxed NC was constructed and the NC phonon modes were calculated. The localisation of the principal (Si-Si, Si-Ge and Ge-Ge) modes ...

Secondary ion mass spectroscopy, Fourier transformed infrared ellipsometry, reflection high energy diffraction and transmission electron microscopy are used to gain inside into the effect of Ge on formation ultrathin 3C-SiC layers Si(111) substrates. Accompanying experimental investigations with simulations it is found that single crystalline layer formed top a gradient Si1–x–yGexCy buffer due ...

We establish an effective theory for heavy-fermion compounds close to a zero temperature antiferromagnetic (AFM) transition. Coming from the heavy Fermi liquid phase across to the AFM phase, the heavy electron fractionalizes into a light electron, a bosonic spinon, and a new excitation: a spinless fermionic field. Assuming this field acquires dynamics and dispersion when one integrates out the ...

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