# 3.2. Carrier effective mass

## 3.2.1. Introduction

The effective mass is a suitable method to describe the density of states and electron transport on semiconductors and insulators materials [W05]. This approach is based on a free electron model and has been proven to be helpful to understand and engineering electronic materials [GRL17].

The effective mass values of the charge carriers are obtained from a free electron-like parabolic fit of band structure extrema. On NanoDCAL, these values are calculated by a finite-difference second order derivative of energy band (\(E\)) with respect to the electron momentum \(k\). The energy of the electron is expanded in a Taylor series around the extrema energy point \(k_{0}\):

The carrier effective mass \(m^{\ast}\) is expressed in unit of rest mass \(m_{0}\) of an electron as:

Since the effective mass is essentially related to the curvature of the dispersion relation, bands of large curvature correspond to small effective masses (light) while flatter bands are related with larger effective masses (heavier).

To compute the effective mass using NanoDCAL code we have to perform the following steps:

Import the crystal;

SCF calculation;

Band structure calculations;

Calculate effective mass.

In the previous section (SOI), we already learned how:

Import the Si crystal using Device Studio software (step 1);

Set and execute the SCF calculation (step 2);

How to calculate and plot the band structure of Silicon (step 3).

From the step 3, we can analyze the \(E-k\) diagram and choose the \(k\)-direction in which the effective mass will be calculated.

## 3.2.2. Effective mass calculation

The required input files for the effective mass calculation of Si could be generated using Device Studio with NanoDCAL module simulator, as follows:

In the menu bar of Device Studio, click

**Simulator**➟**NanoDCAL**➟**Analysis**to pop up the interface where the user could set physical quantities that will be calculated;Navigate to the

**Analysis**panel (left side) ➟ select**EffectiveMass**➟ click on the*Right arrow*button to transfer**EffectiveMass**calculator to the**Calculation Selected**panel.

In the

**EffectiveMass**panel (right side) two rows are used to set the band and \(k\)-path used in the numerical differentiation for electron and hole carriers.

Set the the values according the table below and click **Generate files**.

hole |
-1 |
1 |
1/2 1/2 1/2 |
1/2 1/2 1/2 |

electron |
-1 |
1 |
1/2 1/2 1/2 |
1/2 1/2 1/2 |

Below we’ll briefly discuss the specified keywords. Before running the calculation, make sure that you understand how this parameters will affect the results.

Effective mass input file

```
system.object = NanodcalObject.mat
calculation.name = effectiveMass
calculation.effectiveMass.massParameters = { 'hole',-1,1,[0 0 0],[1/2 1/2 1/2],;'electron',1,1,[0 0 0],[0 1/2 1/2]}
```

The keywords specifies the following:

`system.object`

If it is not empty, the system is defined by the input object. In this case, all other parameters related to the system in the input file will not be used.`calculation.name`

The description must be provided to invoke the kind of calculation`calculation.effectiveMass.massParameters`

. The user should set:The charge carrier: hole or electron.

The energy band information or

*band index*, where: 1 represents the bottom of the conduction band, 2 represents the sub-conduction band; -1 represents the top of the valence band, and -2 represents the sub-valence band.The

*spin information*, where 1 represents spin-up and 2 represents spin-down. For**NoSpin**or**GeneralSpin**calculation, this value is 1.The \(k\)-points coordinates (represented by fractional coordinates), used to define the \(k\)-path.

Important

NanoDCAL will compute the band structure along the \(k\)-path, find the minimum (for electrons) and maximum (for holes), and perform a quadratic fit at the extremer. The quadratic fit is performed along the \(k\)-direction set by the \(k\)-path and its two transverse directions, which means that the charge carriers effective masses will be also calculated along those directions.

Run the simulation with the EffectiveMass input file (`EffectiveMass.input`

). After the calculations, the .mat data files could be loaded in MATLAB platform to extract the effective mass results.

## 3.2.3. Effective mass for Si

The output file has the following information:

The calculated results for effective mass of electrons (\(m^{\ast}_{n}/m_{0}\)) and holes (\(m^{\ast}_{p}/m_{0}\)) will be localized at the first and second lines of the output file, respectively;

For each band index, three masses are written in the output. These three masses are the eigenvalues of the effective mass tensor.

In this example, silicon have anisotropic effective masses for electrons and holes. The following discussion will be based on the band structure plot of silicon crystal, which can be viewed here.

Tip

In this example the effective mass calculation was performed for several band indices. The user should modify the \(k\) path and *band index* according to the system.

Valence band masses (holes)

The highest occupied state (valence band maximum) is localized at the \(\Gamma\)-point. Thus, the corresponding effective masses of holes were calculated between \(\Gamma\)-point [0 0 0] and \(L\)-point [1/2 1/2 1/2]. The three-fold degenerated valence bands are indexed as:

Heavy-hole (HH) for band indices -1 and -2;

Light-hole (LH) for band index -3.

The calculated hole effective masses are showed below:

band index |
effective mass |
mass_l |
mass_t1 |
mass_t2 |
---|---|---|---|---|

-1 |
HH |
0.684 |
0.776 |
2.481 |

-2 |
HH |
0.684 |
0.394 |
0.266 |

-3 |
LH |
0.098 |
0.107 |
0.111 |

Note

The mass_l was calculated along the longitudinal \(k\) path direction.

The mass_t1 was calculated along the first transverse direction

The mass_t2 was calculated along the second transverse direction

Conduction band masses (Electrons)

The lowest unoccupied band appears along the \(\Gamma\)-point [0 0 0] and \(X\)-point [1/2 0 1/2], around \(0.85X\). The electron effective mass eigenvalues are presented below:

band index |
effective mass |
mass_l |
mass_t1 |
mass_t2 |
---|---|---|---|---|

1 |
electron |
0.9262 |
0.194 |
0.194 |

## 3.2.4. Density of states effective mass

The occupation of electrons in a solid is defined by the Fermi surface, which is a direct consequence of the Pauli exclusion principle. The density of state effective mass (\(m^{*}_{dos}\)) essentially maps the volume of the Fermi surface and affects the Seebeck coefficient calculation. So, for a semiconductor material the description of \(m^{*}_{dos}\) is of paramount importance.

The \(m^{*}_{dos}\) is related to the diagonal elements of the mass tensor (\(m_{1}\), \(m_{2}\), and \(m_{3}\)). Most of the band structures from semiconductors have ellipsoidal energy surfaces, resulting in different longitudinal (\(m^{*}_{l}\)) and transversal (\(m^{*}_{t}\)) effective masses. The density-of-states effective mass is expressed as:

where \(M_{c}\) is the number of equivalent band minima.

The density-of-states effective mass for Si

For instance, the silicon possess 6-fold valley degeneracy (\(M_{c}=6\)), with two equivalent directions (the transverse direction) and one longitudinal direction. The \(m^{*}_{dos}\) value for silicon was calculate to be:

## 3.2.5. Conductivity effective mass

The material conductivity is inversely proportional to the effective masses. In this case, a simple conductivity effective mass \(m^{*}_{C}\) could be defined to estimate the electron mobility of semiconductor materials. The conductivity due to multiple band maxima or minima is proportional to the sum of the inverse of the individual masses multiplied by the density of carriers in each band. The resulting effective mass \(m^{*}_{C}\) expression is given by:

The effective mass for conductivity in Si

For silicon crystal, we found

Important

The carrier effective mass analyses for silicon could be improved if spin-orbit effects were taken into account. The user should be able to modify the input files and repeat the calculations to improve accuracy of these results.

Wasserman. Effective masses J. Phys. Condens. Matter. (2005) p. 1-5.

Gibbs, F. Ricci, G.g Li, H. Zhu, K. Persson, G. Ceder, G. Hautier, A. Jain, G. J. Snyder. Effective mass and Fermi surface complexity factor from ab initio band structure calculations npj Comput. Mater. 3, (2017) p. 1-8.