/*! This file is auto-generated */ .wp-block-button__link{color:#fff;background-color:#32373c;border-radius:9999px;box-shadow:none;text-decoration:none;padding:calc(.667em + 2px) calc(1.333em + 2px);font-size:1.125em}.wp-block-file__button{background:#32373c;color:#fff;text-decoration:none} Problem 10 Assume that the \(\mathrm{Cu}\) ... [FREE SOLUTION] | 91Ó°ÊÓ

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Assume that the \(\mathrm{Cu}\) concentration in \(\mathrm{SiO}_{2}\) layer is \(5 \times 10^{13}\) atoms/cm \(^{3}\) after vapor phase decomposition and is measured with atomic absorption spectrometry. The \(\mathrm{Cu}\) concentration in the \(\mathrm{Si}\) layer is \(3 \times 10^{11}\) atoms \(/ \mathrm{cm}^{3}\) after \(\mathrm{HF} / \mathrm{H}_{2} \mathrm{O}_{2}\) dissolution. Calculate the segregation coefficient of \(\mathrm{Cu}\) in \(\mathrm{SiO}_{2} / \mathrm{Si}\) layers.

Short Answer

Expert verified
The segregation coefficient of Cu in \(\mathrm{SiO}_{2} / \mathrm{Si}\) layers is approximately 166.7.

Step by step solution

01

Identifying the given values

In this step, we identify the given values and assign them symbols for easy reference. Given values: - The concentration of Cu in \(\mathrm{SiO}_{2}\) layer-\(C_{\mathrm{SiO}_{2}} = 5 \times 10^{13} \, \mathrm{atoms/cm}^{3}\) - The concentration of Cu in \(\mathrm{Si}\) layer-\(C_{\mathrm{Si}} = 3 \times 10^{11} \, \mathrm{atoms/cm}^{3}\)
02

Calculate the segregation coefficient

Now that we have the values of the Copper concentration in both layers, we can use the segregation coefficient formula: \[K = \frac{C_{\mathrm{SiO}_{2}}}{C_{\mathrm{Si}}}\] Substitute the values of \(C_{\mathrm{SiO}_{2}}\) and \(C_{\mathrm{Si}}\): \[K = \frac{5 \times 10^{13}}{3 \times 10^{11}}\]
03

Simplify the expression

In this step, we will simplify the expression to get the value of the segregation coefficient: \[K = \frac{5 \times 10^{13}}{3 \times 10^{11}} = \frac{5}{3} \times \frac{10^{13}}{10^{11}} = \frac{5}{3} \times 10^{2}\]
04

Finalize the answer

Now that we have simplified the expression, the segregation coefficient of Cu in \(\mathrm{SiO}_{2} / \mathrm{Si}\) layers is: \[K = \frac{5}{3} \times 10^{2} \approx 166.7\] Hence, the segregation coefficient of Cu in \(\mathrm{SiO}_{2} / \mathrm{Si}\) layers is approximately 166.7.

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Key Concepts

These are the key concepts you need to understand to accurately answer the question.

Segregation Coefficient
The segregation coefficient, often denoted as \( K \), is a measure of how a particular element or impurity distributes itself between two adjacent phases, such as two different layers in a semiconductor device. In this context, it is used to understand how copper (Cu) disperses between the silicon dioxide (SiOâ‚‚) and silicon (Si) layers within a semiconductor device.
The segregation coefficient is calculated as the ratio of the concentration of an element in one phase to its concentration in another. In mathematical terms for our scenario, it is expressed as:
  • \( K = \frac{C_{\mathrm{SiO}_2}}{C_{\mathrm{Si}}} \)
This equation helps determine how well integrated an impurity is within the layered structure. A higher \( K \) value suggests that the impurity prefers staying in the SiO₂ layer rather than in the Si layer. In our example, with \( C_{\mathrm{SiO}_2} = 5 \times 10^{13} \) atoms/cm³ and \( C_{\mathrm{Si}} = 3 \times 10^{11} \) atoms/cm³, the segregation coefficient is approximately 166.7, indicating a strong preference for copper to reside in the SiO₂ layer.
SiO2/Si Layers
The structure and functionality of SiOâ‚‚/Si layers are fundamental in semiconductor device physics. Silicon dioxide layers, commonly known as oxide layers, are crucial for insulating different regions within the semiconductor and aid in the fabrication of devices such as transistors. When copper diffuses into these layers, its concentration can significantly affect the device's performance.
The SiOâ‚‚ layer acts as a barrier to electron flow, preventing unwanted electrical conduction between different regions of a device. Meanwhile, the underlying Si layer is where the main electronic activity typically occurs. Understanding how impurities like copper segregate between SiOâ‚‚ and Si is essential for device reliability and performance.
The interaction between SiOâ‚‚ and Si layers not only supports device architecture but also influences the electrical characteristics by impacting the impurity distribution, where an unfavorable distribution could lead to undesirable electrical leakage or reduced device efficiency.
Vapor Phase Decomposition
Vapor phase decomposition is a technique often used for depositing thin films and layers in semiconductor manufacturing. This process involves transforming a substance from a gas or vapor into a solid deposit on a substrate, which is crucial for creating even and uniform layers in advanced semiconductor devices.
In the context of our example, vapor phase decomposition helps to uniformly spread copper (Cu) across the SiOâ‚‚ layer. It ensures that the copper atoms are distributed evenly, which is critical for consistently maintaining the electrical properties of the resulting oxide layer.
This process is integral in preparing high-purity layers and controlling the composition of functional materials in modern electronics. Ensuring uniformity and precision during vapor phase decomposition directly impacts the device's performance and longevity, making it an essential aspect of semiconductor fabrication.
Atomic Absorption Spectrometry
Atomic absorption spectrometry (AAS) is an analytical technique used to measure the concentration of elements in a sample with high precision. It operates on the principle of measuring the absorption of light, which is specific to each element, allowing for their quantification even in small concentrations.
In semiconductor applications, AAS is vital for quantifying impurities such as copper in SiOâ‚‚/Si layers. The technique involves vaporizing the sample in a flame or graphite furnace, then measuring the light absorbed by the excited atoms. This absorption correlates directly with the concentration of the element present.
The high sensitivity of AAS makes it ideal for verifying the distribution of elements post-fabrication, ensuring semiconductor devices meet rigorous quality standards. Accurate measurements provided by AAS help in determining the segregation coefficient, as observed in our example, allowing for better control over the semiconductor manufacturing process.

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Most popular questions from this chapter

We would like to form \(0.1 \mu \mathrm{m}\) deep, heavily doped junctions for the source and drain regions of a submicron MOSFET. Compare the options that are available to introduce and activate dopant for this application. Which option would you recommend and why?

Calculate the junction depth and the total amount of dopant introduced after boron predeposition performed at \(950^{\circ} \mathrm{C}\) for 30 minutes in a neutral ambient. Assume the substrate is \(n\)-type silicon with \(N_{D}=1.8 \times 10^{16} \mathrm{~cm}^{-3}\) and the boron surface concentration is \(C_{S}=1.8 \times 10^{20} \mathrm{~cm}^{-3}\).

If arsenic is diffused into a thick slice of silicon doped with \(10^{15}\) boron atoms \(/ \mathrm{cm}^{3}\) at a temperature of \(900^{\circ} \mathrm{C}\) for 3 hours, what is the final distribution of arsenic if the surface concentration is held fixed at \(4 \times 10^{18}\) atoms \(/ \mathrm{cm}^{3}\) ? What is the junction depth? Assume \(D \quad D_{0} e^{\frac{E a}{k T}} \times \frac{n}{n_{i}}, D_{0} \quad 45.8 \mathrm{~cm}^{2} / \mathrm{s}, E a \quad 4.05 \mathrm{eV}, x_{j} \quad 1.6 \sqrt{D t}\)

If a \(50 \mathrm{keV}\) boron ion is implanted into the silicon substrate, calculate the damage density. Assume silicon atom density is \(5.02 \times 10^{22}\) atoms/cm \(^{3}\), the silicon displacement energy is \(15 \mathrm{eV}\), the range is \(2.5 \mathrm{~nm}\), and the spacing between silicon lattice planes is \(0.25 \mathrm{~nm}\).

Explain why high-temperature RTA is preferable to low-temperature RTA for defect-free shallow-junction formation.

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