Big Chemical Encyclopedia

Chemical substances, components, reactions, process design ...

Articles Figures Tables About

Nuclear reactions exit channel

What do we typically measure when we study a nuclear reaction We might measure aR, the total reaction cross section. This might be measured by a beam attenuation method ( transmitted vs- incident) or by measuring all possible exit channels for a reaction where... [Pg.264]

Knowledge of fission and its consequences is important for the nuclear power industry and the related fields of nuclear waste management and environmental cleanup. From the point of view of basic research, fission is interesting in its own right as a large-scale collective motion of the nucleus, as an important exit channel for many nuclear reactions, and as a source of neutron-rich nuclei for nuclear structure studies and use as radioactive beams. [Pg.300]

Not only is the electron-spin state conserved in all these reactions but also the nuclear spin state. Hence, the nuclear spin polarizations present in the pairs are transferred into the diamagnetic products, where they can be detected. Those nuclear spin configurations that slowed down intersystem crossing are over-populated in the product(s) of the exit channel on the same side as the entry channel of the scheme those that accelerated it are overpopulated in the product(s) of the exit channel on the other side. [Pg.87]

The importance of different exit channels can hardly be overstressed. If both exit channels lead to the same product, the spin sorting is undone, and no S-Tq-t)q)e CIDNP results. However, a difference of reaction probabilities suffices for some CIDNP to remain. Another important factor avoiding a cancellation that would otherwise be perfect is nuclear spin relaxation in longer-lived paramagnetic intermediates, free radicals or triplet molecules. Even if there is a complete cancellation of the polarizations at long times but an imbalance of reaction rates, CIDNP occurs as a transient effect and can be detected in a time-resolved experiment. [Pg.87]

This is basically the mechanism described for the dyads of Section 6.6. Spin sorting occurs in the usual way but would be undone by the fact that singlet and triplet exit channels lead to the same product. If, however, the triplet is long lived (e.g. some lOOgs in reaction centres of Rhodobacter sphaeroides P26), a part of its nuclear spin polarizations is destroyed by relaxation, so the cancellation is not perfect, and CIDNP of the singlet exit channel dominates. [Pg.139]

The most fascinating development in this field of CIDNP within the last years has been the observation, by Zysmilich and McDermott [146], of nuclear spin polarized (solid state) 15NNMR spectra from photosynthetic reaction centers in which the forward electron transfer from the primary charge-separated state to the accepting quinone was blocked. The all-emissive polarizations were proposed to be due to a radical pair mechanism, though many of the details are still not very clear. The reaction scheme is virtually identical to that of Chart VIII (Section V.A.2), the donor D being the special pair and the acceptor A the pheophytin. As in that example, the polarizations from the triplet exit channel are hidden in the triplet product 3D for the lifetime of the latter. This feature, in combination with the fact that nuclear spin relaxation in the molecular triplet localized on the special pair is relatively fast, serves to avoid the cancellation of CIDNP that would occur otherwise because the products from both exit channels are identical. [Pg.154]

Such a process may be described as the system passing from the entrance channel (reactants) to the exit channel (products) on the electronic energy map as a function of the nuclear coordinates. For reaction A -I- BC... [Pg.964]

Experimentally, evidence for a target-projectile interaction can be gained from measuring the probability for formation of the products that populate the various exit channels. This information then serves as the basis for interpretation of the reaction mechanism through which a nuclear collision proceeds. It may also provide essential data for nuclear astrophysics, as described in Chap. 12 of Vol. 2, and for evaluating and implementing nuclear applications, discussed in Chaps. 38 and 39 of Vol. 4). [Pg.159]

One of the most sensitive tests of any nuclear reaction model is its success in reproducing absolute doubly differential cross sections d cr/df2 d . In order to obtain the differential cross section for a given exit channel, it is necessary to integrate over the full kinetic energy distribution of the emitted particles at a specific angle. [Pg.160]

In this arrangement, the bombarding beam is led to the air through an exit foil located at the exit of the beam channel behind the coUimator set as shown in O Fig. 33.2b. Exit window can be made of thin beryllium, aluminum, or synthetic Kapton foil. Beam bombardment of the metal foils will generate high y-ray background from nuclear reactions therefore, Kapton foils are sometimes preferred in spite of their shorter lifetime. [Pg.1702]

The (d, ot) reactions are preferred over the (d, p) reactions because the later have low stopping power for incident deuterons and exit proton channels and are thus not suitable for depth profiling. Differential cross-sections for nuclear reactions i N(d, ps) N, i N(d,po)i5N, i4N(d, cco) 2C and i N(d,ai)i2c induced by deuterons from 0.5 to 2 MeV have been reported by Pellegrino et al. (2004). [Pg.275]

In a strict sense, spallation is a nuclear fragmentation process in which the target nucleus loses several nucleons. As used in cosmochem-istry, however, the term is used more broadly to designate the product of any nuclear transformation induced by cosmic rays, primary or secondary, whether produced by spallation in the strict sense or by more specific reaction channels involving fewer exiting particles (e.g., (p,pn) or (n, a) reactions). [Pg.386]

We denote the entrance and exit reaction channels by a and 3, respectively. In space-fixed coordinates, denoted by (xyz), the inter-nuclear distance vector of the reactant molecule is r and the vector of the colliding atom with respect to the centre of mass of the diatomic molecule is Ry. The angle between y and Ry is y. We define the mass-scaled coordinates... [Pg.334]


See other pages where Nuclear reactions exit channel is mentioned: [Pg.6]    [Pg.33]    [Pg.92]    [Pg.92]    [Pg.96]    [Pg.106]    [Pg.138]    [Pg.147]    [Pg.157]    [Pg.214]    [Pg.274]    [Pg.964]    [Pg.288]    [Pg.20]    [Pg.49]    [Pg.141]   
See also in sourсe #XX -- [ Pg.24 ]




SEARCH



Exitation

Exiting

Exits

Nuclear reaction channels

Nuclear reactions

Reaction channel

© 2024 chempedia.info