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[Author] Tatsuya NAKAMURA(2hit)

1-2hit
  • Low Loss Magnetic Plate Application for Increasing Radiation Efficiency of Cellular Telephones

    Eiji HANKUI  Tatsuya NAKAMURA  Osamu HASHIMOTO  

     
    PAPER-Microwaves, Millimeter-Waves

      Vol:
    E84-C No:6
      Page(s):
    814-822

    A low loss magnetic plate positioned near an antenna is proposed to increase radiation efficiency of cellular phones. This magnetic plate is used to control the nearby magnetic field around the cellular phone's antenna, and this field controlling is shown to be effective for the improvement of radiation efficiency and far-field pattern. As for the material design of the plate, a magnetic plate having high µr and low µr" (complex relative permeability: µr = µr - j µr") is found to be effective for achieving high performance. In our sample fabrication, a low loss magnetic sample with µr = 5.7 - j 0.7 at 900 MHz is realized. It is demonstrated that this low loss sample contributes to increased efficiency and improved far-field characteristics.

  • Current and Radiation Noise up to GHz Band Generated by Slowly Breaking Silver-Compound Contacts

    Yoshiki KAYANO  Tatsuya NAKAMURA  Kazuaki MIYANAGA  Hiroshi INOUE  

     
    LETTER-Signal Transmission & Sensing

      Vol:
    E90-C No:7
      Page(s):
    1504-1506

    To clarify the mechanism of the generation of electromagnetic (EM) noise, current and radiation noise up to the GHz band generated by slowly breaking silver-compound contacts were investigated experimentally. The current and radiation noise at the GHz band were observed. It was demonstrated that the frequency spectrums of the current and radiation noise correspond to the frequency responses of the circuit admittance and radiation efficiency of the experimental setup, respectively. It was revealed that even if current noise at the GHz band is very small, it can cause a large EM radiation noise because of the high radiation efficiency. From the time-frequency domain characteristics of current noise, it was clarified that the peaks of current noise at 10 MHz band arise immediately after the initiation of the arc discharge and the transition from metallic phase to gaseous phase. On the other hand, the peak current noise above 100 MHz arises immediately after the initiation of the arc discharge.

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