<xml>
  <records>
    <record>
       <contributors>
          <authors>
             <author>Hsieh, C.-Y.</author>
             <author>Chen, S.-H.</author>
             <author>Lin, M.W.</author>
          </authors>
       </contributors>
       <titles>
          <title>
             Modeling of Self-Modulated Laser Wakefield Acceleration Driven by Sub-Terawatt Laser Pulses
          </title>
       </titles>
		 <publisher>JACoW Publishing</publisher>
       <pub-location>Geneva, Switzerland</pub-location>
		 <isbn>978-3-95450-184-7</isbn>
		 <electronic-resource-num>10.18429/JACoW-IPAC2018-THPML018</electronic-resource-num>
		 <language>English</language>
		 <pages>4690-4692</pages>
       <pages>THPML018</pages>
       <keywords>
       </keywords>
       <work-type>Contribution to a conference proceedings</work-type>
       <dates>
          <year>2018</year>
          <pub-dates>
             <date>2018-06</date>
          </pub-dates>
       </dates>
       <urls>
          <related-urls>
              <url>https://doi.org/10.18429/JACoW-IPAC2018-THPML018</url>
              <url>http://jacow.org/ipac2018/papers/thpml018.pdf</url>
          </related-urls>
       </urls>
       <abstract>
          Laser wakefield accelerator (LWFA) can be achieved in a scheme in which a sub-terawatt (TW) laser pulse is introduced into a thin, high-density target*. As a result, the self-focusing and the self-modulation can greatly enhance the peak intensity of the laser pulse capable of exciting a nonlinear plasma wave to accelerate electrons. A particle-in-cell model was developed to study the sub-TW LWFA, in which a 0.6-TW laser pulse is injected into a hydrogen gas cell with a flat-top density profile. In addition to using 800-nm laser pulses, laser pulses of 1030 nm were used in simulations as they represent a viable approach to realize the sub-TW LWFA driven by high-frequency, diode-pumped laser systems**. Process of the electron injection is complicated in such a high-density plasma; however, the simulation results show that the appropriate injection and acceleration of electrons can be achieved by optimizing the length of the gas cell. When a 340-micrometer long gas cell is introduced, energetic electrons (&gt; 1 MeV) are produced with a relatively low emittance of 3.5 pi-mm-mrad and a total charge of 0.32 nC accordingly.
       </abstract>
    </record>
  </records>
</xml>
