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2.6.1 Contrast and Important Properties

The performance of any photoresist can be characterized by its contrast curve. The contrast curve describes the remaining resist fraction of a uniformly illuminated resist versus the logarithm of the applied exposure dose. Idealized contrast curves for positive and negative resists are shown in Figure 2.7. The contrast $ \gamma$ is given by the expression [23, p. 187]

$\displaystyle \gamma = \frac{1}{\displaystyle\log_{10}\frac{D_{100}}{D_0}},$ (2.6)

with doses D100 and D0 defined in Figure 2.7. It is a simple measure of how well the resist can convert the distorted patterns of a ``blurred'' aerial image into a ``sharp'' binary stencil. Clearly, a high-contrast resist increases the resolution of the entire lithography process by reducing the parameter k1 in (2.1). Typical values for $ \gamma$ range from 2-3. Hence, D100 is 101/3 to 101/2 times lager than D0, e.g., D0$ \le$50 mJ/cm2 and D100$ \ge$150 mJ/cm2. As the exposure dose depends on the exposure intensity as well as on the exposure time both quantities have to be chosen accordingly to transfer the pattern into the resist. The contrast crucially depends on all of the resist processing steps described in Section 2.6.3. The absorption spectrum and the bleaching behavior are also of great influence. Furthermore, second order effects like surface reflection and a non-uniform resist thickness have to be taken into account.


  
Figure 2.7: The contrast curve is a logarithmic sensitivity plot showing resist thickness versus exposure energy. The contrast $ \gamma$ is defined as the linear slope of the transition region and describes the ability of the resist to distinguish between light and dark areas.
\resizebox{8cm}{!}{
\psfrag{D100}{\tiny$D_{100}$ }
\psfrag{D0}{\tiny$D_{0}$ }
\includegraphics{PRresistcontrast.eps}}

In the following list some important resist properties are summarized [24, p. 204]:


next up previous contents
Next: 2.6.2 Composition of DQN Up: 2.6 Photoresist Previous: 2.6 Photoresist
Heinrich Kirchauer, Institute for Microelectronics, TU Vienna
1998-04-17