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Nascent fragments

DNA synthesis in the lower arm of the diagram (on the 5 —>3 template) is made in the direction opposite to fork movement and in short segments of 100-1,000 nucleotides in length. These are called Okazaki or nascent fragments. Thus replication of both arms can be represented as shown in Fig. 16-11. [Pg.466]

A characteristic feature of the DNA polymerases is their inability to initiate synthesis of a polydeoxynucleotide chain they can only extend an existing chain. How is initiation of the nascent fragments within the discontinuously synthesized DNA strand achieved ... [Pg.484]

Hydrocarbon molecules are abundant constituents of planetary atmospheres and major compounds in combustible gas mixtures and in fusion edge plasmas [7-11]. Methane is the simplest of these hydrocarbon molecules. Acetylene, C2H2, is the simplest hydrocarbon molecule that contains 2 carbon atoms. Thus absolute total and partial photon [24-27] and electron [15,28-34] ionization cross-sections and nascent fragment ion energy distributions [19,20,28,36-40] have been studied extensively for these molecules. For the deuterated methane molecule electron impact ionization and dissociative ionization cross-sections were determined for the CD (x=l—4) molecule and radicals applying a fast neutral beam technique [41]. Electron impact total ionization cross-sections have been determined also theoretically applying the BEB (Binary-Encounter-Bethe) model [42], the DM (Deutsch-Mark) method [43] and the JK (Jain-Khare) method [44], Partial electron impact ionization cross-sections were calculated for methane [45,46] as well as total electron impact cross-sections for various CH radicals [47]. The dissocia-... [Pg.439]

The probed nascent fragment population traveling with a distribution of velocities will give rise to a Doppler profile about v0. Analysis of this profile can lead to a state-specific P(Etrans) for the photodissociation process [31,44-50], A variation of Doppler spectroscopy can be accomplished by measuring a series of Doppler profiles and changing the delay time between the PUMP and the PROBE steps between each measurement. This technique, known as velocity-aligned Doppler spectroscopy (VADS), is a more direct observation of the speed distribution of the probed molecule along kpr, rather than just a measurement of the velocity components in this direction [51]. As is clear from the above theoretical... [Pg.293]

To see the nascent fragments it is most convenient to ionize them. This can be done by a UV laser and, in common with other spectroscopic techniques, it can be done in a state-selective manner. In Section 7.1.2.3 we adopted this feature by using a (right or left) circularly polarized laser ionization beam to discern the orientation of the electronic angular momentum of the Cl fragment formed in the dissociation of ICl. [Pg.285]

If the metastable decomposition occurs in flight before the ion reaches the analyser of a mass spectrometer, a typical metastable peak may be observed in the mass spectrum depending on the type of mass analyser used. Moreover, using appropriate methods, it is also possible to deduce the kinetic energy distribution of the nascent fragment ions at these late times after the initial excitation. [Pg.1016]

DNAIigase Seals the single strand nick between the nascent chain and Okazaki fragments on lagging strand... [Pg.328]

The temporal resolution of both methods is limited by the risetime of the IR detectors and preamplifiers, rather than the delay generators (for CS work) or transient recorders (SS) used to acquire the data, and is typically a few hundred nanoseconds. For experiments at low total pressure the time between gas-kinetic collisions is considerably longer, for example, approximately 8 /is for self-collisions of HF at lOmTorr. Nascent rotational and vibrational distributions of excited fragments following photodissociation can thus be obtained from spectra taken at several microseconds delay, subject to adequate SNR at the low pressures used. For products of chemical reactions, the risetime of the IR emission will depend upon the rate constant, and even for a reaction that proceeds at the gas-kinetic rate the intensity may not reach its maximum for tens of microseconds. Although the products may only have suffered one or two collisions, and the vibrational distribution is still the initial one, rotational distributions may be partially relaxed. [Pg.29]


See other pages where Nascent fragments is mentioned: [Pg.28]    [Pg.4]    [Pg.300]    [Pg.318]    [Pg.325]    [Pg.328]    [Pg.485]    [Pg.289]    [Pg.86]    [Pg.20]    [Pg.139]    [Pg.977]    [Pg.979]    [Pg.224]    [Pg.14]    [Pg.28]    [Pg.4]    [Pg.300]    [Pg.318]    [Pg.325]    [Pg.328]    [Pg.485]    [Pg.289]    [Pg.86]    [Pg.20]    [Pg.139]    [Pg.977]    [Pg.979]    [Pg.224]    [Pg.14]    [Pg.872]    [Pg.3043]    [Pg.327]    [Pg.97]    [Pg.15]    [Pg.404]    [Pg.406]    [Pg.23]    [Pg.289]    [Pg.322]    [Pg.475]    [Pg.44]    [Pg.19]    [Pg.167]    [Pg.271]    [Pg.165]    [Pg.168]    [Pg.1051]    [Pg.25]    [Pg.27]    [Pg.35]    [Pg.36]    [Pg.36]    [Pg.62]    [Pg.70]    [Pg.655]   
See also in sourсe #XX -- [ Pg.466 ]




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