Post by QuantumDiamonds

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"𝗎𝗞𝘂ð—ŋ ð—ŋð—ē𝘀𝗞ð—đ𝘂𝘁ð—ķ𝗞ð—ŧ ð—ķ𝘀 𝟭 Ξ𝗚 ð—Ŋ𝘂𝘁 𝗞𝘂ð—ŋ ð—ģð—Ūð—ķð—đ𝘂ð—ŋð—ē𝘀 ð—Ūð—ŋð—ē 𝟭𝟎𝟎 ð—ŧ𝗚" It sounds obvious: if your imaging resolution is 1 Ξm, how could you detect a defect ten times smaller? The physics works in your favor here, because we measure 𝘁ð—ĩð—ē 𝗚ð—Ūð—īð—ŧð—ē𝘁ð—ķ𝗰 ð—ģð—ķð—ēð—đð—ą 𝗞ð—ģ 𝘁ð—ĩð—ē 𝗰𝘂ð—ŋð—ŋð—ēð—ŧ𝘁, ð—ŧ𝗞𝘁 𝘁ð—ĩð—ē 𝘀𝘁ð—ŋ𝘂𝗰𝘁𝘂ð—ŋð—ē ð—ķ𝘁𝘀ð—ēð—đð—ģ. Apply a current, and it follows every path it can. A short adds a path that should not exist. An open stops the current where the connection breaks. Both show up as a clear anomaly in the magnetic map, so the same measurement ð—ģð—ķð—ŧð—ąð˜€ 𝘀ð—ĩ𝗞ð—ŋ𝘁𝘀 ð—Ūð—ŧð—ą ð—žð—―ð—ēð—ŧ𝘀 ð—Ūð—đð—ķð—ļð—ē. And the signal does not stay small. As the field travels up through the package, it spreads out: a 100 nm feature under a 10 Ξm stack leaves a magnetic imprint several microns wide. But ð—Ū 𝘄ð—ķð—ąð—ēð—ŋ 𝘀ð—ķð—īð—ŧð—Ūð—đ ð—ķ𝘀 ð—ŧ𝗞𝘁 ð—Ū 𝘃ð—Ūð—ī𝘂ð—ēð—ŋ 𝗞ð—ŧð—ē. Where it peaks, how it falls off, which way the current turns, all of it is ð—Ū ð—ģð—ķð—ŧð—īð—ēð—ŋð—―ð—ŋð—ķð—ŧ𝘁 𝗞ð—ģ 𝘁ð—ĩð—Ū𝘁 ð—ģð—Ūð—ķð—đ𝘂ð—ŋð—ē ð˜ð˜†ð—―ð—ē ð—Ū𝘁 𝘁ð—ĩð—Ū𝘁 ð˜€ð—―ð—ē𝗰ð—ķð—ģð—ķ𝗰 ð—đ𝗞𝗰ð—Ū𝘁ð—ķ𝗞ð—ŧ. We read that fingerprint and reconstruct the current path to a precise position in X, Y, and Z. That is what the QDm.1 puts to use: ð—Ū 𝟭 Ξ𝗚 ð—ŋð—ē𝘀𝗞ð—đ𝘂𝘁ð—ķ𝗞ð—ŧ 𝘀𝘆𝘀𝘁ð—ē𝗚 ð—đ𝗞𝗰ð—Ūð—đð—ķ𝘇ð—ē𝘀 ð—Ū 𝟭𝟎𝟎 ð—ŧ𝗚 ð—ąð—ēð—ģð—ē𝗰𝘁, ð—ŧ𝗞ð—ŧ-ð—ąð—ē𝘀𝘁ð—ŋ𝘂𝗰𝘁ð—ķ𝘃ð—ēð—đ𝘆, deep inside an optically opaque 2.5D or 3D package. Resolution tells you how sharply you see the field. It is not the limit on the feature size you can find. More on the method, and the measurements behind it, via the links in the comments.

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