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Donor Impurities When an impurity contains an excess of electrons, the dopant is called a donor impurity Adding such a substance causes conduction mainly by means of electron flow, as in an ordinary metal such as copper or aluminum The excess electrons are passed from atom to atom when a voltage exists across the material Elements that serve as donor impurities include antimony, arsenic, bismuth, and phosphorus A material with a donor impurity is called an N-type semiconductor, because electrons have negative (N) charge Acceptor Impurities If an impurity has a deficiency of electrons, the dopant is called an acceptor impurity When a substance such as aluminum, boron, gallium, or indium is added to a semiconductor, the material conducts by means of hole flow A hole is a missing electron or more precisely, a place in an atom where an electron should be, but isn t A semiconductor with an acceptor impurity is called a P-type semiconductor, because holes have, in effect, a positive (P) charge Majority and Minority Carriers Charge carriers in semiconductor materials are either electrons, each of which has a unit negative charge, or holes, each of which has a unit positive charge In any semiconductor substance, some

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In this approach, the receiver clock error is augmented to the navigation state and estimated The augmented model is x = [n, e, , RL , RR , c tr , c tr ] x = [ n, e, , RL , RR , c tr , c tr ] According to eqn (849), the clock estimate is propagated through time as c tr (k) = c tr (k 1) + c tr (k 1) Tk (925)

The pseudorange and carrier phase measurements are de ned in eqns (86) and (825) Based on those equations, the pseudorange and carrier phase measurements can be predicted from the navigation state as i i x R( , pi ) + c tr + i i x = R( , p ) + c tr + i + N i = (926) (927)

of hole flow Solid black dots represent electrons, moving in one direction Open circles represent holes, moving in the opposite direction

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where the measurements are assumed to be simultaneous and the time arguments have been dropped to simplify the notation Note that prediction of the carrier phase measurements assumes that estimates of the carrier phase integer ambiguities N i are available The discussion below assumes that the integer estimates are correct and available If the integer ambiguities are incorrect, the phase measurements would be biased by an integer number

of wavelengths If the integer ambiguities are not available, then the phase measurements are not used Alternatively, the phase measurements could be used either to smooth the pseudoranges or through temporal di erencing to estimate the velocity In this approach, the measurement residuals for the i-th satellite are computed as i (t) i (t) i i (t) i (t) (t) = i (t) = The error models for the measurement residuals are i (t) (t)

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