Specific Process Knowledge/Lithography/Coaters/Spin Coater: RCD8 processing: Difference between revisions
Created page with "=Spin coating= The process of spin coating on Spin Track 1 + 2 consists of a selection of the following steps: *Acceleration to a low spin speed if dynamic dispense is used *R..." |
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=Spin coating= | =Spin coating= | ||
The process of spin coating on Spin | The process of spin coating on Spin Coater: RCD8 consists of a selection of the following steps: | ||
*Acceleration to a low spin speed if dynamic dispense is used | *Acceleration to a low spin speed if dynamic dispense is used | ||
*Resist dispense | *Resist dispense | ||
*Closing the Gyrset | |||
*Resist spreading at low spin speed | *Resist spreading at low spin speed | ||
*Spin-off | *Spin-off | ||
*Deceleration | *Deceleration | ||
* | *Opening Gyrset | ||
The wafer is first centered on the | The wafer is first centered on the chuck and held in place by vacuum (or pins in the case of the non-vacuum chuck). If static dispense is used, the spindle remains static during the ensuing resist dispense. In the case of dynamic dispense, the spindle is accelerated to a low spin speed before the resist is dispensed. Using too high spin speed during dispense can cause surface wetting issues, while a too low spin speed causes the resist to flow onto the backside of the wafer. The resist may be dispensed manually, or automatically using the syringe dispense system on the media arm. After dispense, a short spin at low spin speed may be used in order to spread the resist over the wafer surface before spin-off. | ||
The spin-off cycle determines the thickness of the resist coating. The thickness is primarily a function of the spin-off speed and the spin-off time, both following an inverse power-law (y=k*x^-a). The acceleration to the spin-off speed also influences the thickness, but the effect is dependent on previous steps. The spin-off is usually a simple spin at one speed, but it may be comprised of several steps at different spin speeds. After spin-off, the wafer is decelerated. | The spin-off cycle determines the thickness of the resist coating. The thickness is primarily a function of the spin-off speed and the spin-off time, both following an inverse power-law (y=k*x^-a). The acceleration to the spin-off speed also influences the thickness, but the effect is dependent on previous steps. The spin-off is usually a simple spin at one speed, but it may be comprised of several steps at different spin speeds. After spin-off, the wafer is decelerated. | ||
The coated thickness, t, as a function of the spin-off speed, w, follows an inverse power-law t=k*w^-a. The constant, k, is a function of the resist viscosity and solid content, and the spin-off time. The exponent, a, is dependent on solvent evaporation, and is usually ½. This means that using the thickness t1 achieved at spin speed w1, one can estimate the thickness t2 at spin speed w2 using the relation <br> t1*w1^2 = t2*w2^2 => t2 = t1 * w1^2/w2^2 <br> | |||
=Automatic dispense= | =Automatic dispense= |
Revision as of 09:33, 27 April 2015
Spin coating
The process of spin coating on Spin Coater: RCD8 consists of a selection of the following steps:
- Acceleration to a low spin speed if dynamic dispense is used
- Resist dispense
- Closing the Gyrset
- Resist spreading at low spin speed
- Spin-off
- Deceleration
- Opening Gyrset
The wafer is first centered on the chuck and held in place by vacuum (or pins in the case of the non-vacuum chuck). If static dispense is used, the spindle remains static during the ensuing resist dispense. In the case of dynamic dispense, the spindle is accelerated to a low spin speed before the resist is dispensed. Using too high spin speed during dispense can cause surface wetting issues, while a too low spin speed causes the resist to flow onto the backside of the wafer. The resist may be dispensed manually, or automatically using the syringe dispense system on the media arm. After dispense, a short spin at low spin speed may be used in order to spread the resist over the wafer surface before spin-off.
The spin-off cycle determines the thickness of the resist coating. The thickness is primarily a function of the spin-off speed and the spin-off time, both following an inverse power-law (y=k*x^-a). The acceleration to the spin-off speed also influences the thickness, but the effect is dependent on previous steps. The spin-off is usually a simple spin at one speed, but it may be comprised of several steps at different spin speeds. After spin-off, the wafer is decelerated.
The coated thickness, t, as a function of the spin-off speed, w, follows an inverse power-law t=k*w^-a. The constant, k, is a function of the resist viscosity and solid content, and the spin-off time. The exponent, a, is dependent on solvent evaporation, and is usually ½. This means that using the thickness t1 achieved at spin speed w1, one can estimate the thickness t2 at spin speed w2 using the relation
t1*w1^2 = t2*w2^2 => t2 = t1 * w1^2/w2^2