Variation of the electron energy distribution with He dilution in an inductively coupled argon discharge

We present experimental evidence of different behaviors of plasma parameters depending on changes in the electron energy distribution (EED), caused by an electron heating mechanism and electron-neutral collision processes in an Ar/He mixture inductively coupled plasma. At a low gas pressure of 3 mTorr, where the electron neutral collision frequency νm is much smaller than the driving frequency ωRF, the EEDs evolved from a bi-Maxwellian distribution to a Maxwellian distribution, due to the efficient heating of low energy electrons when the He flow rate increased at a fixed total gas pressure. The plasma density slowly decreased with the He flow rate portion ([He]/[Ar] + [He]) in a range of 0%–70%, while the plasma density largely decreased in the He flow rate portion of 70%–100%. On the other hand, at a high gas pressure of 350 mTorr where νm ≫ ωRF, the EEDs evolved from a Druyvesteyn-like distribution to a Maxwellian distribution, due to a cooling of low energy electrons and an increase in the population ...

[1]  C. Chung,et al.  Experimental measurements of spatial plasma potentials and electron energy distributions in inductively coupled plasma under weakly collisional and nonlocal electron kinetic regimes , 2012 .

[2]  R. Gottscho Plasma Etching - The Challenges Ahead in Enabling Nanoelectronics , 2011 .

[3]  Wei Jiang,et al.  Collisionless bounce resonance heating in dual-frequency capacitively coupled plasmas. , 2011, Physical review letters.

[4]  L. Tsendin Nonlocal electron kinetics in gas-discharge plasma , 2010 .

[5]  C. Chung,et al.  Evolution of the electron energy distribution and E-H mode transition in inductively coupled nitrogen plasma , 2010 .

[6]  C. Chung,et al.  Experimental observation of the transition from nonlocal to local electron kinetics in inductively coupled plasmas , 2010 .

[7]  C. Chung,et al.  Low energy electron heating and evolution of the electron energy distribution by diluted O2 in an inductive Ar/O2 mixture discharge , 2010 .

[8]  C. Chung,et al.  Observation of collisionless heating of low energy electrons in low pressure inductively coupled argon plasmas , 2008 .

[9]  K. Ostrikov,et al.  Electron/ion energy loss to discharge walls revised : a case study in low-temperature, thermally nonequilibrium plasmas , 2008 .

[10]  S. S. Kim,et al.  Gap length effect on electron energy distribution in capacitive radio frequency discharges , 2007 .

[11]  Seungkyu Ahn,et al.  Driving frequency effect on electron heating mode transition in capacitive discharge , 2006 .

[12]  C. Theodosiou,et al.  Elastic electron scattering from inert-gas atoms , 2005 .

[13]  D. Tsiklauri,et al.  Phase mixing of shear Alfvén waves as a new mechanism for electron acceleration in collisionless, kinetic plasmas , 2004, astro-ph/0409537.

[14]  H. Sugai,et al.  Electron heating mode transition observed in a very high frequency capacitive discharge , 2003 .

[15]  C. Chung,et al.  Heating-mode transition in the capacitive mode of inductively coupled plasmas , 2002 .

[16]  S. S. Kim,et al.  Electron cyclotron resonance in a weakly magnetized radio-frequency inductive discharge. , 2002, Physical review letters.

[17]  H. Uhm,et al.  Electron temperature analysis of two-gas-species inductively coupled plasma , 2001 .

[18]  Jon Tomas Gudmundsson,et al.  On the effect of the electron energy distribution on the plasma parameters of an argon discharge : a global (volume-averaged) model study , 2001 .

[19]  Hong-young Chang,et al.  Electron energy distribution function and plasma potential in a planar inductive argon discharge without electrostatic screen , 1999 .

[20]  N. Braithwaite,et al.  Tailoring of electron energy distributions in low-pressure inductive discharges , 1999 .

[21]  Vladimir Kolobov,et al.  EFFECT OF COLLISIONLESS HEATING ON ELECTRON ENERGY DISTRIBUTION IN AN INDUCTIVELY COUPLED PLASMA , 1998 .

[22]  J. Palop,et al.  A new smoothing method for obtaining the electron energy distribution function in plasmas by the numerical differentiation of the I‐V probe characteristic , 1995 .

[23]  U. Kortshagen,et al.  On the efficiency of the electron sheath heating in capacitively coupled radio frequency discharges in the weakly collisional regime , 1995 .

[24]  Hopkins,et al.  Anomalous sheath heating in a low pressure rf discharge in nitrogen. , 1992, Physical review letters.

[25]  I. Kaganovich,et al.  The space-time-averaging procedure and modeling of the RF discharge II. Model of collisional low-pressure RF discharge , 1992 .

[26]  Benjamin Alexandrovich,et al.  Measurement of electron energy distribution in low-pressure RF discharges , 1992 .

[27]  Graves,et al.  Electron acoustic waves in capacitively coupled, low-pressure rf glow discharges. , 1991, Physical review letters.

[28]  Godyak,et al.  Abnormally low electron energy and heating-mode transition in a low-pressure argon rf discharge at 13.56 MHz. , 1990, Physical review letters.

[29]  J. Boeuf,et al.  A Monte Carlo analysis of an electron swarm in a nonuniform field: the cathode region of a glow discharge in helium , 1982 .