No abstract

Much interest has recently centred on the properties of peptides that modulate the excitability of nerve cells. Such compounds include the undecapeptide substance P, which is particularly well established as an excitatory neurotransmitter, and we examine here its effects on magnocellular cholinergic neurones taken from the medial and ventral aspects of the globus pallidus of newborn rats and grown in dissociated culture. These neurones have previously been shown to respond to substance P3 and are analogous to the nucleus basalis of Meynert in man, which gives a diffuse projection to the cerebral cortex and whose degeneration is the likely cause of Alzheimer's disease. Substance P depolarizes these cultured neurones by reducing an inwardly rectifying potassium conductances; this conductance has been found in several neuronal types and has similar properties to those of certain other cells. As discussed below, modulation of inward (or anomalous) rectification by substance P implies a self-reinforcing element to the depolarization caused by the peptide.

We demonstrate that fiber-based frequency combs with multi-branch configurations can transfer both linewidth and frequency stability to another wavelength at the millihertz level. An intra-cavity electro-optic modulator is employed to obtain a broad servo bandwidth for repetition rate control. We investigate the relative linewidths between two combs using a stable continuous-wave laser as a common reference to stabilize the repetition rate frequencies in both combs. The achieved energy concentration to the carrier of the out-of-loop beat between the two combs was 99% and 30% at a bandwidth of 1 kHz and 7.6 mHz, respectively. The frequency instability of the comb was 3.7x10(-16) for a 1 s averaging time, improving to 5-8x10(-19) for 10000 s. We show that the frequency noise in the out-of-loop beat originates mainly from phase noise in branched optical fibers.

No abstract

We demonstrate a one-dimensional optical lattice clock with ultracold 171 Yb atoms, which is free from the linear Zeeman effect. The absolute frequency of the 1 S 0 ðF ¼ 1=2Þ-3 P 0 ðF ¼ 1=2Þ clock transition in 171 Yb is determined to be 518 295 836 590 864(28) Hz with respect to the SI second.