RF discharge-based plasma emitter

An injector of hydrogen atoms for plasma diagnostics in modern tokamaks has been developed at the Budker Institute of Nuclear Physics (Novosibirsk). The ion source of the injector produces a proton (helium ion) beam with a current of up to 2 A (1 A), an ion energy of up to 55 keV, a beam divergence of ～0.6\deg, and a pulse duration of up to 10 s. An RF discharge-based plasma emitter, which is one of the main parts of the ion source, is described. The emitter diameter is 72 mm, the ion current density is 120 mA/cm², and the inhomogeneity of the current density is ±6%. The beam is formed by a four-electrode ionoptical system with 163 round apertures. At a current of 2 A, the ion beam consists of 67% protons, 18% H ₂ ⁺ ions, and 15% H ₃ ⁺ ions, the total content of heavier ions in the beam being no higher than 2–3%.     

RF lesion generation.

Although the technique of RF lesion generation is a well-established medical technique, most professionals using it do not understand the basic principles of electronics by which the phenomenon occurs. A review of this with special attention to the 'indifferent' or 'dispersive' electrode would lead to better practice and less adverse effects, such as patient skin burns.     

RF absorption involving biological macromolecules

The fundamental intramolecular frequency of a globular protein can be obtained from the measurements of acoustic velocities of bulk protein matter. This lowest frequency for common size molecules is shown to be above several hundred GHz. All modes below this frequency would then be intermolecular modes or bulk modes of the molecule and surrounding matter or tissue. The lowest frequency modes of an extended DNA double helix are also shown to be bulk modes because of interaction with water. Only DNA modes, whose frequency is well above 4 GHz, can be intrahelical modes, that is, confined to the helix rather than in the helix plus surroundings. Near 4 GHz, they are heavily damped and, therefore, not able to resonantly absorb. Modes that absorb radio frequency (RF) below this frequency are bulk modes of the supporting matter. Bulk modes rapidly thermalize all absorbed energy. The implication of these findings for the possibility of athermal RF effects is considered. The applicability of these findings for other biological molecules is discussed.     

Stop codon recognition and interactions with peptide release factor RF3 of truncated and chimeric RF1 and RF2 from Escherichia coli

Release factors RF1 and RF2 recognize stop codons present at the A-site of the ribosome and activate hydrolysis of peptidyl-tRNA to release the peptide chain. Interactions with RF3, a ribosome-dependent GTPase, then initiate a series of reactions that accelerate the dissociation of RF1 or RF2 and their recycling between ribosomes. Two regions of Escherichia coli RF1 and RF2 were identified previously as involved in stop codon recognition and peptidyl-tRNA hydrolysis. We show here that removing the N-terminal domain of RF1 or RF2 or exchanging this domain between the two factors does not affect RF specificity but has different effects on the activity of RF1 and RF2: truncated RF1 remains highly active and able to support rapid cell growth, whereas cells with truncated RF2 grow only poorly. Transplanting a loop of 13 amino acid residues from RF2 to RF1 switches the stop codon specificity. The interaction of the truncated factors with RF3 on the ribosome is defective: they fail to stimulate guanine nucleotide exchange on RF3, recycling is not stimulated by RF3, and nucleotide-free RF3 fails to stabilize the binding of RF1 or RF2 to the ribosome. However, the N-terminal domain seems not to be required for the expulsion of RF1 or RF2 by RF3:GTP.     

Natural electrical RF oscillation from cells

Electrical oscillatory rf phenomena are present during the division of cells. These were examined by studying the attraction of cells for polarizable powders. They are understood to occur by a process termed microdielectrophoresis (-DEP), the motion induced by a nonuniform electric field acting on a polarizable body. The suggestion that an electrical oscillatory aspect may also be involved in the contact or density inhibition of cell division and the mechanisms that may cause invasiveness of oncogenic cells are theoretically explored (i.e., changes in either the power level or the frequency of the oscillatory phenomena associated with cell division, or in the degree of electrical insulation of the cell from electrical damping by nearby cells). A number of experiments to test this hypothesis are suggested.     

Protein synthesis factors (RF1, RF2, RF3, RRF, and tmRNA) and peptidyl-tRNA hydrolase rescue stalled ribosomes at sense codons

During translation, ribosomes stall on mRNA when the aminoacyl-tRNA to be read is not readily available. The stalled ribosomes are deleterious to the cell and should be rescued to maintain its viability. To investigate the contribution of some of the cellular translation factors on ribosome rescuing, we provoked stalling at AGA codons in mutants that affected the factors and then analyzed the accumulation of oligopeptidyl (peptides of up to 6 amino acid residues, oligopep-)-tRNA or polypeptidyl (peptides of more than 300 amino acids in length, polypep-)-tRNA associated with ribosomes. Stalling was achieved by starvation for aminoacyl-tRNA(Arg4) upon induced expression of engineered lacZ (β-galactosidase) reporter gene harboring contiguous AGA codons close to the initiation codon or at internal codon positions together with minigene ATGAGATAA accompanied by reduced peptidyl-tRNA hydrolase (Pth). Our results showed accumulations of peptidyl-tRNA associated with ribosomes in mutants for release factors (RF1, RF2, and RF3), ribosome recycling factor (RRF), Pth, and transfer-messenger RNA (tmRNA), implying that each of these factors cooperate in rescuing stalled ribosomes. The role of these factors in ribosome releasing from the stalled complex may vary depending on the length of the peptide in the peptidyl-tRNA. RF3 and RRF rescue stalled ribosomes by "drop-off" of peptidyl-tRNA, while RF1, RF2 (in the absence of termination codon), or Pth may rescue by hydrolyzing the associated peptidyl-tRNA. This is followed by the disassembly of the ribosomal complex of tRNA and mRNA by RRF and elongation factor G.     

Release factor RF3 in E.coli accelerates the dissociation of release factors RF1 and RF2 from the ribosome in a GTP-dependent manner.

Ribosomes complexed with synthetic mRNA and peptidyl-tRNA, ready for peptide release, were purified by gel filtration and used to study the function of release factor RF3 and guanine nucleotides in the termination of protein synthesis. The peptide-releasing activity of RF1 and RF2 in limiting concentrations was stimulated by the addition of RF3 and GTP, stimulated, though to a lesser extent, by RF3 and a non-hydrolysable GTP analogue, and inhibited by RF3 and GDP or RF3 without guanine nucleotide. With short incubation times allowing only a single catalytic cycle of RF1 or RF2, peptide release activity was independent of RF3 and guanine nucleotide. RF3 hydrolysis of GTP to GDP + P(i) was dependent only on ribosomes and not on RF1 or RF2. RF3 affected neither the rate of association of RF1 and RF2 with the ribosome nor the catalytic rate of peptide release. A model is proposed which explains how RF3 recycles RF1 and RF2 by displacing the factors from the ribosome after the release of peptide.     

Comparative study of translation termination sites and release factors (RF1 and RF2) in procaryotes

Translation termination is catalyzed by release factors that recognize stop codons. However, previous works have shown that in some bacteria, the termination process also involves bases around stop codons. Recently, Ito et al. analyzed release factors and identified the amino acids therein that recognize stop codons. However, the amino acids that recognize bases around stop codons remain unclear. To identify the candidate amino acids that recognize the bases around stop codons, we aligned the protein sequences of the release factors of various bacteria and searched for amino acids that were conserved specifically in the sequence of bacteria that seemed to regulate translation termination by bases around stop codons. As a result, species having several highly conserved residues in RF1 and RF2 showed positive correlations between their codon usage bias and conservation of the bases around the stop codons. In addition, some of the residues were located very close to the SPF motif, which deciphers stop codons. These results suggest that these conserved amino acids enable the release factors to recognize the bases around the stop codons. Present address (Y. Ozawa): Tokyo Research Laboratory, IBM Japan, Ltd., 1623-14 Shimotsuruma, Yamato-shi, Kanagawa 242-8502, Japan     

Methylation of bacterial release factors RF1 and RF2 is required for normal translation termination in vivo

Bacterial release factors RF1 and RF2 are methylated on the Gln residue of a universally conserved tripeptide motif GGQ, which interacts with the peptidyl transferase center of the large ribosomal subunit, triggering hydrolysis of the ester bond in peptidyl-tRNA and releasing the newly synthesized polypeptide from the ribosome. In vitro experiments have shown that the activity of RF2 is stimulated by Gln methylation. The viability of Escherichia coli K12 strains depends on the integrity of the release factor methyltransferase PrmC, because K12 strains are partially deficient in RF2 activity due to the presence of a Thr residue at position 246 instead of Ala. Here, we study in vivo RF1 and RF2 activity at termination codons in competition with programmed frameshifting and the effect of the Ala-246 --> Thr mutation. PrmC inactivation reduces the specific termination activity of RF1 and RF2(Ala-246) by approximately 3- to 4-fold. The mutation Ala-246 --> Thr in RF2 reduces the termination activity in cells approximately 5-fold. After correction for the decrease in level of RF2 due to the autocontrol of RF2 synthesis, the mutation Ala-246 --> Thr reduced RF2 termination activity by approximately 10-fold at UGA codons and UAA codons. PrmC inactivation had no effect on cell growth in rich media but reduced growth considerably on poor carbon sources. This suggests that the expression of some genes needed for optimal growth under such conditions can become growth limiting as a result of inefficient translation termination.     

Magnetic field measurements near RF induction heaters

We discuss initial magnetic field strength measurements made around radiofrequency (RF) induction heaters. These measurements were made with a monitor developed for the National Institute for Occupational Safety and Health (NIOSH) by the National Bureau of Standards (NBS). The monitor has a dynamic range of .01 to 10,000 A2/m2, a frequency range of 300 kHz to 100 MHz, an isotropic response (+/- .3 dB) with three mutally orthogonal loop antennas that have the ability to measure and display each of three orthogonal magnetic field components, a high probe burnout protection level of 20,000 A2/m2, and an accuracy of +/- 1.0 dB at 13 calibration frequencies. The portable survey monitor was used to measure the magnetic field strengths in the vicinity of 16 RF induction heaters. Typically these induction heaters are operated continuously for several hours. The maximum field strengths (without duty factor correction) ranged from 15 to 4,500 A2/m2 and were measured 5 to 51 cm from the loop applicators of the induction heaters. At locations commonly occupied by workers (ie, approximately 30 to 76 cm from heaters), the fields ranged from .01 to 300 A2/m2 (without duty factor correction).     

RF Exposure During Use of Electrosurgical Units

Electrosurgical units (ESUs) commonly used in operating suites employ radiofrequency (RF) energy for cutting and coagulation, and operate at different frequencies in the range 0.3–5 MHz. Around the electrode and cables, electric and magnetic fields at similar frequencies will be generated, and the surgeon using the ESU will therefore be exposed to these electromagnetic fields. In this study we have measured the levels of RF fields near the lead wires of two electrosurgical units, BARD 3000 operating at a fixed frequency of 0.5 MHz, and ERBE ICC 350 with a frequency range from 0.3 to 1 MHz. Electric fields were measured at distances from 5–30 cm from the lead wire. Measurements were done with the ESU both cutting and coagulating, and power levels ranging from 10–100 W. The magnetic field outside the lead wire was calculated from the measured current through the leads using standard theory. Using those measurements as a base, the calculated local exposure of the surgeon's hand was estimated to exceed 15 kV/m for the electric field and the corresponding value for the magnetic field was 16 µT. These calculations exceed the suggested international reference levels at 0.5 MHz (610 V/m and 4 µT, respectively).     

Numerical dosimetry dedicated to children RF exposure

Children are more and more using wireless communication systems. This growth has strengthened public concern and has highlighted the need to assess the radio frequency (RF) exposure of children. In dosimetry, taking advantage of the improvement of High Performance Calculation systems, great efforts have been carried out to improve the numerical tools and human models used to assess the Specific Absorption Rate (SAR). This paper analyses progress in building child and foetus models for numerical dosimetry purpose. The simulation results, in terms of Specific Absorption Rate over 1 and 10 g of tissues, in specific organs such as brain and averaged over the whole body, are reported and analysed. The results show that compliance methods used nowadays to certify phones are valid for children. The studies also show that specific tissues such as peripheral brain tissues can have higher exposure with children than with adults. Studies performed with plane waves as sources and whole body children models show that the whole body SAR of children can be higher than the WBSAR of adults and that the compliance to ICNIRP reference levels does not guarantee the compliance to ICNIRP basic restrictions. Dealing with the foetus models and dielectric properties great efforts have been made. Preliminary results show that the foetus exposure is often lower than the mother exposure, with an important influencing parameter: the foetus position in the uterus.     

ArfA Recruits RF2 into Stalled Ribosomes

During translation in Escherichia coli, the ribosome rescue factor YaeJ and the alternative ribosome rescue factor (ArfA, previously called YhdL) can release stalled ribosomes from mRNA. Here, I used a reconstituted cell-free protein synthesis system to examine YaeJ- and ArfA-dependent recycling of stalled ribosomes, in which mRNA lacks in-frame stop codons. It is shown that YaeJ alone could recycle the ribosome but that ArfA required the presence of release factor 2 (RF2). Furthermore, I show that RF2 binds to stalled ribosomes only in the presence of ArfA, demonstrating that ArfA recruits RF2 into the A site of the ribosome to facilitate peptidyl-tRNA hydrolysis. It is also demonstrated that the efficiency of the ArfA-dependent process decreases rapidly with an increase in mRNA length downstream of the A site of the ribosome whereas YaeJ function is maintained on mRNA with sufficient length. From the results, I discuss differences of in vivo roles of these two systems in addition to the well-known tmRNA-dependent trans-translation system.     

Perspectives with cryogenic RF probes in biomedical MRI

Since discovery of high-temperature superconductive (HTS) ceramics by Bednorz and Muller in 1986, there has been an accelerated development of cold technologies in industry, including the domain of NMR detection. The purpose of this paper is to fix ideas about the stage that cryogenic radio frequency (RF) probe techniques have reached in biomedical magnetic resonance imaging (MRI). Readers confronted to the literature about this emerging topic have to understand a large range of motivations with somewhat unclearly defined technical limitations and actual outlets. An overview of sensitivity issues in the general context of biomedical MRI is provided here and the contribution of RF coil techniques to recent advances is identified. The domains where cooled coil materials such as copper, low- or high-temperature superconductors, could actually increase the RF coil sensitivity are delimited by a quantitative analysis of noise mechanisms. Technical keys, cryogenic means and cold RF coil technologies are considered, and first achievements in different fields of biomedical MRI are reviewed. This survey provides a basis for discussing about the future impact of cryogenic probes for MRI investigations.     

Ribosome release factor RF4 and termination factor RF3 are involved in dissociation of peptidyl-tRNA from the ribosome.

Peptidyl-tRNA dissociation from ribosomes is an energetically costly but apparently inevitable process that accompanies normal protein synthesis. The drop-off products of these events are hydrolysed by peptidyl-tRNA hydrolase. Mutant selections have been made to identify genes involved in the drop-off of peptidyl-tRNA, using a thermosensitive peptidyl-tRNA hydrolase mutant in Escherichia coli. Transposon insertions upstream of the frr gene, which encodes RF4 (ribosome release or recycling factor), restored growth to this mutant. The insertions impaired expression of the frr gene. Mutations inactivating prfC, encoding RF3 (release factor 3), displayed a similar phenotype. Conversely, production of RF4 from a plasmid increased the thermosensitivity of the peptidyl-tRNA hydrolase mutant. In vitro measurements of peptidyl-tRNA release from ribosomes paused at stop signals or sense codons confirmed that RF3 and RF4 were able to stimulate peptidyl-tRNA release from ribosomes, and showed that this action of RF4 required the presence of translocation factor EF2, known to be needed for the function of RF4 in ribosome recycling. When present together, the three factors were able to stimulate release up to 12-fold. It is suggested that RF4 may displace peptidyl-tRNA from the ribosome in a manner related to its proposed function in removing deacylated tRNA during ribosome recycling.     

Generic UMTS test signal for RF bioelectromagnetic studies

This report outlines the characteristics of universal mobile telecommunications system (UMTS) signals and discusses the signal parameters with respect to their possible biological relevance in order to define a generic UMTS test signal (GUS) for experiments aiming at the investigation of biological effects of weak electromagnetic fields. The GUS includes features of a real UMTS signal and especially the characteristics of UMTS, which differ from those of already applied second generation mobile communication systems (GSM 900, DCS1800, PCS1900, IS-95). It has been specified on the basis of the recommendations of a working group of the German Forschungsgemeinschaft Funk (FGF) with a focus on the mechanisms of UMTS which are responsible for slow term signal contributions, i.e., low frequency variations of the radio frequency (RF) envelope, since the hypothetical possibility of biological relevance of weak electromagnetic fields is often attributed to time variations of the RF envelope with frequencies close to those of natural processes. In this respect, it is also shown that the mandatory power control loop in UMTS gives rise to very strong 1.5 kHz variations on the air interface. Based upon the concept of the GUS, a UMTS test signal generator (GUS6960S) is described.     

射频热疗技术在脑胶质瘤治疗中的应用进展

近几年,射频(radio frequency,RF)热疗技术以其靶向、微创、效果好,副作用少等特点,在临床治疗中,尤其是恶性肿瘤的治疗方面,取得了巨大的发展。随着研究的逐步深入,射频热疗技术越来越受到人们的重视,其应用范围也逐渐宽泛。脑胶质瘤呈广泛侵袭性生长,尤其是Ⅲ～Ⅳ级胶质瘤,具有高度间变的生长特点,术后复发快,手术加放化疗的平均生存期仅为8～11个月,严重威胁人类健康,是神经外科治疗领域中最难治疗的肿瘤。因而有关恶性脑胶质细胞瘤发生、发展及治疗的研究一直是神经外科领域的热点之一。本文就射频热疗技术的基本原理、脑胶质瘤治疗现状、射频热疗技术在脑胶质瘤治疗方面的应用,最新研究方向及进展做一综述。     

Low-power inductive RF plasma sources for technological applications

The objective of the present paper is to develop an analytic theory of cylindrical low-power RF plasma sources operating at an industrial frequency (f=13.56 MHz, ω=8.52×10⁷ s^?1). Inductive surface exciters of electromagnetic fields (exciting antennas) are considered that are positioned either at the side surface of the cylinder or at one of its end surfaces. In the latter case, the plasma flows out of the source through the opposite end surface of the cylinder. A study is made of elongated systems in which the length L of the cylinder exceeds its diameter 2R and of planar disk-shaped systems with L<2R. Simple analytic expressions are derived for electromagnetic fields excited by the antenna in the source plasma. The equivalent plasma resistance and the equivalent RF power deposited in the plasma are calculated for systems with prescribed parameters, i.e., in a non-self-consistent model. Up to now, such sources have been investigated mainly through the numerical solution of the complicated general electrodynamic equations. In the Introduction, the problem is formulated in general terms and the geometry of the sources, as well as the characteristic parameters of the source plasma, is discussed. In Section 2, plasma sources operating without an external magnetic field are investigated. In Section 3, helicon plasma sources in a sufficiently strong external magnetic field are considered. Analytic predictions are compared with the results from solving the problem numerically without using the helicon approximation. Section 4 gives a brief discussion of an electron cyclotron resonance-based RF plasma source. In the Conclusion, the main results of the paper are summarized and the technological efficiency of the sources under consideration is estimated at a qualitative level.     

Low-current moderate-pressure RF discharge with secondary electron photoemission

A model is proposed for a low-current RF discharge with secondary electron photoemission from the electrode surface caused by photons originating in the electrode sheath. The low-current state of RF discharges at moderate pressures is peculiar in that the electrons and ions produced during the preceding periods of the RF field promote the development of the discharge during subsequent periods. Since the ion space charge is induced during many periods of the RF field, even comparatively moderate fields in the electrode sheath are sufficient to ensure the conditions under which the current is self-sustaining, in which case the electron photoemission dominates over the remaining secondary processes at the electrode surface. In a low-current RF discharge, the ion-electron emission has essentially no impact on the formation of the electrode sheath because the half-period of the RF field is much shorter than the ion transit time through the sheath. The sheath results from the overlap of the secondary electron avalanches triggered by electron photoemission from the electrode surface. The sheath parameters are determined by the conditions under which the current in the sheath is selfsustaining due to the secondary electron photoemission from the electrode surface. The capacitive susceptance of the electrode sheath is substantially higher than its electrical conductance. Low-current RF discharges can only exist when the time required for the ions to drift through the sheath and reach the electrode is much longer than the half-period of the RF field.