It incorporates the latest Lame MP3 Encoder 3.97 encoding algorithms which generate crisp tantalizing quality audio. This Sound Normalizer is simple to use with fast and excellent quality results. The Sound Normalizer also allows editing ID3 tags (build-in Mp3 ID3 Tag Editor) with support for ID3v1 and ID3v2 tags, converting Wav to Mp3 files and Mp3 to Wav files (build-in Wav/Mp3 Converter) using Lame MP3 Encoder 3.97, listening Mp3 and Wav files using the build-in audio player. The Mp3 Normalizer allows to modify the volume of a scanned file directly without usage tags. The mp3 normalization is fulfilled under standard Replay Gain. The mp3 normalization and test is fulfilled on an average level (RMS normalization). The wav normalization and test is fulfilled on a peak level (Peak Normalization). The level of volume and normalization is represented graphically and in percentage. It contains batch processor and it allows to fulfill the batch test, batch normalization and batch converting of Mp3 and Wav files. It is reached by the test and normalization of the level volume of Mp3 and Wav files. The time from production to analysis of an isotope has thereby been reduced to 10/sup -6/ s while it was 10/sup -1/ to 10/sup 0/ s for He-jets and 10/sup 1/ to 10/sup 3/ s for rapid chemical separations.The Sound Normalizer improves and regains a quality of Mp3 and Wav (PCM 8, 16, 24, 32 bits, DSP, GSM, IMA ADPCM, MS ADPCM, AC3, MP3, MP2, OGG, A-LAW, u-LAW) files. cap alpha.-spectrometry has been coupled with the magnetic analysis of the recoils. For the synthesis of element 106 an aerosol-based recoil transport technique was devised. Many variations of these methods have been developed and are discussed. Subsequent electrical deposition or a He-jet technique yielded samples that were not only thin enough for. These were based on the large momentum transfer associated with heavy-ion reactions, which produced energetic target recoils that, when ejected from the target, could be thermalized in He gas. With the advent of heavy-ion accelerators new sample preparation methods emerged. cap alpha.-spectrometry more » were prepared by chemical methods. Up to mendelevium (Z = 101), thin samples suitable for. This technique has been used for all recent discoveries of new elements including Z = 109. cap alpha.-emission of daughter and granddaughter nuclei. SOUND NORMALIZER V7.99.7 SERIEScap alpha.-decay series led to the very powerful method of genetically linking the decay of new elements to the well-established. cap alpha.-spectra have proved simple to interpret and exhibit systematic trends that allow extrapolation to unknown isotopes. cap alpha.-spectrometry has played a decisive role in the discovery of new, heavy elements. The present talk will summarize the systematical behavior of the Po isotopes and discuss the role of collective excitations. Due to insufficient knowledge of the background spectra, however, the presented evidence should only be regarded as preliminary and tentative. The identification more » of the modulations involves a technique that subtracts the bulk statistical background from the measured alpha spectra, in order for the modulations to become visible in the residuals. Some evidence for the modulations has been observed in the alpha spectra measured in the 3He-induced reactions, 3He + natAg in particular. The optical modulations are expected to arise from the ~-particle interaction with the rest of the nucleus as the particle prepares to exit. In Part II, we report on a search for evidence of the optical modulations in the energy spectra of alpha particles emitted from hot compound nuclei. The upper limits for the transient time set with this new method are 15x 10 –21 sec and 25x 10 –21 sec for 0s and Po compound nuclei, respectively. The upper limits are constrained by the fission probabilities of neighboring isotopes. A novel approach has been developed to determine upper limits of the transient time of the fission process. The fission barriers, and shell effects for the corresponding nuclei are extracted from the detailed analyses. These excitation functions have been analyzed in detail based upon the transition state formalism. In Part I, fission excitation functions of osmium isotopes 185,186, 187, 189 Os produced in 3He + 182,183, 184, 186W reactions, and of polonium isotopes 209,210, 211, 212Po produced in 3He/ 4He + 206, 207, 208Pb reactions, were measured with high precision.
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