Diffused Base 1954 Cool and Inspect Crystal
# Cool and Inspect the Crystal: Why Bulk Defects Matter More When Both Junctions Form Inside Them
This step cools the rod grown in Step 3 and inspects it for defects before any wafer is cut from it — and because this process's two junctions will eventually sit entirely inside whatever bulk crystal this step passes, a dislocation or a region of thermal stress here is not a cosmetic flaw this device can route around. An alloy-junction device's electrical behavior concentrates at the alloyed regrowth interface, a boundary the firing step itself creates fresh; a diffused-base device's two junctions sit wherever the diffusion fronts from Steps 12 through 19 happen to land, inside bulk crystal this step either leaves clean or does not. A dislocation that intersects a future junction plane here becomes a leakage path later, with nothing in the diffusion schedule able to detect or avoid it in advance.
## 1. Cooling Rate Sets a Stress Field This Process Cannot Simply Anneal Away Later
Thermal stress $\sigma_{\text{thermal}}$ during cooling scales with germanium's thermal expansion coefficient $\alpha_{\text{Ge}}$, its elastic modulus $E$, and the radial temperature gradient $dT/dr$ across the cooling rod — too fast a cool leaves that gradient steep and the resulting stress high enough to nucleate dislocations the rod did not have during growth. Those dislocations do not heal themselves during the later diffusion anneals; if anything, a dislocation can act as a fast diffusion path, letting dopant atoms travel preferentially along it and reach depths the surrounding bulk diffusion profile never predicted. A defect this step fails to catch does not stay dormant through two later high-temperature diffusions — it has every opportunity to make itself worse.
## 2. Real Diagram: A Dislocation Waits, Then Becomes a Leakage Path Once Diffusion Reaches It
## 3. Inspection Has to Characterize the Whole Volume, Not Just the Surface This Process Will Later Diffuse Into
Resistivity $\rho(z)$ measured along the rod's length should track the target $\rho_0$ from Step 2 closely, with deviation $\delta\rho(z)$ small and random rather than systematic — but for this process specifically, inspection has to characterize resistivity and structural soundness through the *entire* thickness that will eventually become the finished collector, not just a thin surface skin. Both future diffusions only reach a few micrometers deep; everything beneath that remains exactly what this step either verified or failed to verify, for the full working life of the device.
## Cool and Inspect the Crystal's Place in the Process Lineage
Cooling and inspecting the crystal is step four of Bell Labs' twenty-six-step diffused-base manufacturing sequence — immediately after the single-composition pull finished, and before any section of the rod is judged usable or cut. It is the last point in this entire process where the bulk crystal's defect structure can be checked directly, because every later step either diffuses into a thin surface skin or cuts and handles material whose internal defects this step was the only chance to find. Step five, selecting usable crystal sections, depends entirely on this step's inspection having actually looked deep enough to matter.