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However, all three particles in this equation are fermions with intrinsic spins S 1 h . Therefore, we cannot balance the angular momentum in the reaction as 2 written. The spins of the proton and the electron can be coupled to 0 or 1 h and can also have relative angular momenta with any integral value from the emission process. This simple spin algebra will never yield the half-integral value on the left-hand side of the equation. Another fermion must be present among the products. Another feature of b decay that was puzzling at rst but really pointed to the incompleteness of the previous equation is that the b rays have a continuous energy distribution. That is, electrons are emitted from a source with a distribution of energies that extends from a maximum at the Q value down to zero. Recall that if there are only two products from a reaction then they will precisely share the decay energy according to conservation of momentum. We have clearly seen such sharp energy spectra in a decay. (The continuous energy distribution is not an instrumental artifact, nor does it come from electron scattering.) Quite dramatic pictures of the tracks of charged particles from beta decay show events in which the particles move in one direction in clear violation of conservation of linear momentum. The way out of this mounting paradox with violations of very strongly held conservation laws is to introduce another conservation law and recognize that another unseen particle must be created and emitted. The conservation law is conservation of the number of particles in a reaction, and the unseen particle is a form of neutrino, literally the little neutral one in Italian.

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Data can be streamed in and out of the database as XML or in binary format. Streams can be somewhat dif cult to work with because of their transient nature. Generally, a stream can be consumed once and then it disappears:

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To add a custom repository to Ubuntu, do the following from the Synaptic Package Manager window: 1. Select Settings Repositories. The Software Preferences window appears. 2. Select Add. The Edit Repository window appears. 3. Click Custom. You are asked to add a complete APT line, identifying the repository. 4. Type the line identifying the APT repository that contains the outside software you want to install. (The following is an example of a line identifying a fictitious repository.)

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that is, we get the Geiger Nuttall law of a decay, where a b are constants that depend on Z, and so forth. This simple estimate tracks the general behavior of the observed emission rates over the very large range in nature. The calculated emission rate is typically one order of magnitude larger than that observed, meaning that the observed half-lives are longer than predicted. This has led some researchers to suggest that the probability to nd a preformed a particle inside a heavy nucleus is on the order of 1021 or less. One way to obtain an estimate of the preformation factor is to plot, for even even nuclei undergoing l 0 decay, the ratio of the calculated half-life to the measured half-life. This is done in Figure 7.7. The average preformation factor is 1022.

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release of 10% of the Kr and Xe ssion products as well as some 3H and volatile ssion products. These off-gases are combined with those from the dissolution step. In the dissolution step, the fuel pieces are dissolved in near boiling 10 M HNO3. This step, which takes a few hours, dissolves the uranium, plutonium, and ssion products, leaving the cladding to be recovered. The Kr and Xe are recovered from the off-gas of steam, air, and NOx. The chemical reactions for the dissolution of uranium involve processes like 3UO2 8HNO3 3UO2 (NO3 )2 2NO 4H2 O ! and UO2 4HNO3 UO2 (NO3 )2 2NO2 4H2 O ! The plutonium is oxidized to Pu(IV) and Pu(VI), while the neptunium ends up in the pentavalent or hexavalent states. Small amounts of plutonium and ssion products

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