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believe what the mathematics was telling you because it made no sense physically Mike Lazaridis Scientists around the world, including those at the Perimeter Institute, are starting to gure out how to teleport move atoms from one place to another using quantum mechanics We use a fake form of teleportation today when we phone, fax, or send an e-mail All of these messaging technologies involve making a copy of the original object, sending it to a new location, and then reading it out on the other side Quantum teleportation is a bit like Star Trek s transporter technology, but instead of beaming trillions of atoms down to the planet in a couple of shimmering seconds, physicists are nding they can nudge a few atoms at a time from one place to another instantly Copenhagen scientists using a new method, called a Bose-Einstein condensate, can cause about 5,000 particles to disappear from one place and appear thirty centimeters away At the Perimeter Institute in Waterloo, La amme has been able to manipulate a grand total of seven quantum bits ( qubits ) to run a calculation On the surface, this seems to be the same as scanning a message into pixels, faxing it, and recreating it at the other end, except the scientists are adding in entangled quantum states to send the real thing, not a copy It works something like this: when two atoms or two laser beams are inextricably dependent on each other, ie, entangled, it is possible to make a link between two ends of a line In the case of two entangled particles, if one is rotating in one direction, the other one will always be rotating in the pposite direction and vice versa When you measure one particle, it instantaneously in uences its entangled partner When you act to change the state of one, then the other reacts and makes the same change.

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Many of the new and projected large telescopes operate with a Nasmyth focus using a tertiary mirror at 45 The problem that this introduces to polarimetry with discussion on the measures that can be taken to address the issues has been presented by Tinbergen (2007) It may be noted that an alt-azimuth mounting can be advantageous because any telescope instrumental polarization can be determined by comparing the results obtained for the same star either side of the meridian, the whole optical system suffering rotation around the observed direction as the hour angle changes sign This is common practice in radio astronomy For equatorially mounted telescopes, any polarization produced by the mirrors can be explored and eliminated by rotating the entire elescope tube together with the mirrors In the 1960s, two 2400 Cassegrain rotatable telescopes were specially designed for polarimetric use (see Hiltner & Schild, 1965), and these were instrumental in setting up set of unpolarized standard stars In the Northern Hemisphere (Yerkes Observatory), Appenzeller (1968) made use of the instrument in his survey of the galactic pole and in the Southern Hemisphere (Siding Spring in Australia), an important study was made by Serkowski, Mathewson & Ford (1975) The project established a number of nearby stars of intermediate spectral types for which no linear polarization was detectable within the limits of the measurement error It may also be noted that some of the early investigations of interstellar polarization were conducted with large refractor telescopes Again it would be expected that the circular symmetry of the collection aperture in the form of an objective lens should not introduce any spurious instrumental polarization However, Serkowski (1960) drew attention to the effects of stress birefringence that can occur in the glass material of the lenses The small phase changes that are produced effectively decrease the measured values for the degree of linear polarization Using the 26-inch refractor in Belgrade, Krzemi ski (1959) measured the polarization of 23 n stars with known interstellar 4430 band intensities Comparison with the measurements by Hiltner of the same stars showed that the values were systematically smaller, but that they were reconcilable by considering the Belgrade objective to act as a phase plate with a retardance of 1/14 of a wave According to Serkowski (1960), in view of the thickness of the lenses, such a value of phase delay is not unexpected In some cases, instrumental polarization may have components generated in the optics of the modulator itself, or in the electronic gating of the signal For example, if a rotating wave plate is employed as part of the modulator, as well as its phase delay, it also acts as a weak partial polarizer, this affecting the signal to some degree The opening and closing of gates synchronously with the modulator s position to allow sampling over sections of the oscillatory signal needs to be timed to high accuracy and be free from drift For high accuracy and precision in polarimetric observations, stability of operation is important Such aims are best achieved by having telescopes that are dedicated solely to polarimetry The results published by Kemp s group at the University of Oregon and by the Wisconsin group (see Nordsieck, Babler, Bjorkman, et al, 1992) owe their success to this Unfortunately, this means that available apertures will inevitably be fairly small, limiting such polarimetric studies to the brighter stars.

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