Low-energy electron diffraction

Low-energy electron diffraction (LEED) is a technique for the determination of the surface structure of single-crystalline materials by bombardment with a collimated beam of low energy electrons (20–200 eV)^[1] and observation of diffracted electrons as spots on a fluorescent screen.

Figure 1: LEED pattern of a Si(100) reconstructed surface. The underlying lattice is a square lattice while the surface reconstruction has a 2x1 periodicity. As discussed in the text, the pattern shows that reconstruction exists in symmetrically equivalent domains which are oriented along different crystallographic axes. The diffraction spots are generated by acceleration of elastically scattered electrons onto a hemispherical fluorescent screen. Also seen is the electron gun which generates the primary electron beam. It covers up parts of the screen.

LEED may be used in one of two ways:

Qualitatively, where the diffraction pattern is recorded and analysis of the spot positions gives information on the symmetry of the surface structure. In the presence of an adsorbate the qualitative analysis may reveal information about the size and rotational alignment of the adsorbate unit cell with respect to the substrate unit cell.
Quantitatively, where the intensities of diffracted beams are recorded as a function of incident electron beam energy to generate the so-called I-V curves. By comparison with theoretical curves, these may provide accurate information on atomic positions on the surface at hand.

Historical perspective^[2]

Davisson and Germer's discovery of electron diffraction

The theoretical possibility of the occurrence of electron diffraction first emerged in 1924 when Louis de Broglie introduced wave mechanics and proposed the wavelike nature of all particles. In his Nobel laureated work de Broglie postulated that the wavelength of a particle with linear momentum p is given by h/p, where h is Planck's constant. The de Broglie hypothesis was confirmed experimentally at Bell Labs in 1927 when Clinton Davisson and Lester Germer fired low-energy electrons at a crystalline nickel target and observed that the angular dependence of the intensity of backscattered electrons showed diffraction patterns. These observations were consistent with the diffraction theory for X-rays developed by Bragg and Laue earlier. Before the acceptance of the de Broglie hypothesis diffraction was believed to be an exclusive property of waves.

Davisson and Germer published notes of their electron diffraction experiment result in Nature and in Physical Review in 1927. One month after Davisson and Germer's work appeared, Thompson and Reid published their electron diffraction work with higher kinetic energy (thousand times higher than the energy used by Davisson and Germer) in the same journal. Those experiments revealed the wave property of electrons and opened up an era of electron diffraction study.

Development of LEED as a tool in surface science

Though discovered in 1927, low energy electron diffraction did not become a popular tool for surface analysis until the early 1960s. The main reasons were that monitoring directions and intensities of diffracted beams was a difficult experimental process due to inadequate vacuum techniques and slow detection methods such as a Faraday cup. Also, since LEED is a surface sensitive method, it required well-ordered surface structures. Techniques for the reconstruction of clean metal surfaces first became available much later. In the early 1960s LEED experienced a renaissance as ultra high vacuum became widely available and the post acceleration detection method was introduced. Using this technique diffracted electrons were accelerated to high energies to produce clear and visible diffraction patterns on a fluorescent screen.

It soon became clear that the kinematic (single scattering) theory, which had been successfully used to explain X-ray diffraction experiments, was inadequate for the quantitative interpretation of experimental data obtained from LEED. At this stage a detailed determination of surface structures, including adsorption sites, bond angles and bond lengths was not possible. A dynamical electron diffraction theory which took into account the possibility of multiple scattering was established in the late 1960s. With this theory it later became possible to reproduce experimental data with high precision.

Experimental Setup

In order to keep the studied sample clean and free from unwanted adsorbates, LEED experiments are performed in an ultra-high-vacuum environment (10⁻⁹ mbar).

Figure 2 Diagram of a LEED optics apparatus.

The most important elements in a LEED experiment are:^[2]

A sample holder with the prepared sample
An electron gun
A display system, usually a hemispherical fluorescent screen on which the diffraction pattern can be observed directly
A sputtering gun for cleaning the surface
An Auger electron spectroscopy system in order to determine the purity of the surface.

A simplified sketch of an LEED setup is shown in figure 2.^[3]

Sample preparation

The sample is usually prepared outside the vacuum chamber by cutting a slice of around 1 mm in thickness and 1 cm in diameter along the desired crystallographic axis. The correct alignment of the crystal can be achieved with the help of x-ray methods and should be within 1° of the desired angle.^[4] After being mounted in the UHV chamber the sample is chemically cleaned and flattened. Unwanted surface contaminants are removed by ion sputtering or by chemical processes such as oxidation and reduction cycles. The surface is flattened by annealing at high temperatures. Once a clean and well-defined surface is prepared, monolayers can be adsorbed on the surface by exposing it to a gas consisting of the desired adsorbate atoms or molecules.

Often the annealing process will let bulk impurities diffuse to the surface and therefore give rise to a re-contamination after each cleaning cycle. The problem is that impurities which adsorb without changing the basic symmetry of the surface, cannot easily be identified in the diffraction pattern. Therefore, in many LEED experiments Auger electron spectroscopy is used to accurately determine the purity of the sample.

Electron gun

In the electron gun, monochromatic electrons are emitted by a cathode filament which is at a negative potential, typically 10-600 V, with respect to the sample. The electrons are accelerated and focused into a beam, typically about 0.1 to 0.5 mm wide, by a series of electrodes serving as electron lenses. Some of the electrons incident on the sample surface are backscattered elastically, and diffraction can be detected if sufficient order exists on the surface. This typically requires a region of single crystal surface as wide as the electron beam, although sometimes polycrystalline surfaces such as highly oriented pyrolytic graphite (HOPG) are sufficient.

Detector system

A LEED detector usually contains three or four hemispherical concentric grids and a phosphor screen or other position-sensitive detector. The grids are used for screening out the inelastically scattered electrons. Most new LEED systems use a reverse view scheme, which has a minimized electron gun, and the pattern is viewed from behind through a transmission screen and a viewport. Recently, a new digitized position sensitive detector called a delay-line detector with better dynamic range and resolution has been developed.

The LEED contains a retarding field analyzer to block inelastically scattered electrons. Because only spherical fields around the sampled point are allowed and the geometry of the sample and the surrounding area is not spherical, no field is allowed. Therefore, the first grid screens separates the space above the sample from the retarding field. The next grid is at a potential to block low energy electrons, it is called the suppressor or the gate. To make the retarding field homogeneous and mechanically more stable this grid often consists of two grids. The fourth grid is only necessary when the LEED is used like a tetrode and the current at the screen is measured, when it serves as screen between the gate and the anode.

Using the detector for Auger electron spectroscopy

To improve the measured signal in Auger electron spectroscopy, the gate voltage is scanned in a linear ramp. An RC circuit serves to derive the second derivative, which is then amplified and digitized. To reduce the noise, multiple passes are summed up. The first derivative is very large due to the residual capacitive coupling between gate and the anode and may degrade the performance of the circuit. By applying a negative ramp to the screen this can be compensated. It is also possible to add a small sine to the gate. A high Q RLC circuit is tuned to the second harmonic to detect the second derivative.

Data acquisition

Image 1: LEED pattern of a clean platinum-rhodium (100) (Miller-index) single crystal. Taken in high vacuum using an electron gun with an energy of 85 eV.

Image 2: LEED pattern of CO on platinum-rhodium (100) (Miller-index) surface of a single crystal. Taken in high vacuum using an electron gun with an energy of 94 eV.

A modern data acquisition system usually contains a CCD/CMOS camera pointed to the screen for diffraction pattern visualization and a computer for data recording and further analysis.

The shown images are examples of LEED diffraction patterns. The difference between image 1 and 2 is remarkable; where image 1 is of a clean (100) platinum-rhodium single crystal, and image 2 of the same crystal with CO adsorbed on the surface. The original surface order of the clean crystal is clearly visible in image 1, it shows a C(1x1) structure; the extra spots in image 2 are caused by the CO on the surface and are an example of a C(2x2) structure. The diffraction spots are generated by acceleration of elastically scattered electrons onto a hemispherical fluorescent screen, a retarding field analyzer. In the middle one can see the bright spot of the electron gun which generates the primary electron beam.

Theory

Surface sensitivity

The basic reason for the high surface sensitivity of LEED is that for low-energy electrons the interaction between the solid and electrons is especially strong. Upon penetrating the crystal, primary electrons will lose kinetic energy due to inelastic scattering processes such as plasmon- and phonon excitations as well as electron-electron interactions. In cases where the detailed nature of the inelastic processes is unimportant they are commonly treated by assuming an exponential decay of the primary electron beam intensity, I₀, in the direction of propagation:

${\begin{aligned}I(d)=I_{0}*e^{-d/\Lambda (E)}\end{aligned}}$

Here d is the penetration depth and $\Lambda (E)$ denotes the inelastic mean free path, defined as the distance an electron can travel before its intensity has decreased by the factor 1/e. While the inelastic scattering processes and consequently the electronic mean free path depend on the energy, it is relatively independent of the material. The mean free path turns out to be minimal (5–10 Å) in the energy range of low-energy electrons (20–200 eV).^[1] This effective attenuation means that only a few atomic layers are sampled by the electron beam and as a consequence the contribution of deeper atoms to the diffraction progressively decreases.

Kinematic theory: single scattering

Figure 3: Ewald's sphere construction for the case of diffraction from a 2D-lattice. The intersections between Ewald's sphere and reciprocal lattice rods define the allowed diffracted beams.

Kinematic diffraction is defined as the situation where electrons impinging on a well-ordered crystal surface are elastically scattered only once by that surface. In the theory the electron beam is represented by a plane wave with a wavelength in accordance to the de Broglie hypothesis:

{\begin{aligned}\lambda ={\frac {h}{\sqrt {2mE}}},\qquad \lambda [{\textrm {nm}}]\approx {\sqrt {\frac {1.5}{E[{\textrm {eV}}]}}}\end{aligned}}

The interaction between the scatterers present in the surface and the incident electrons is most conveniently described in reciprocal space. In three dimensions the primitive reciprocal lattice vectors are related to the real space lattice {a, b, c} in the following way:^[5]

{\begin{aligned}{\textbf {a}}^{*}&={\frac {2\pi {\textbf {b}}\times {\textbf {c}}}{{\textbf {a}}\cdot ({\textbf {b}}\times {\textbf {c}})}},\\{\textbf {b}}^{*}&={\frac {2\pi {\textbf {c}}\times {\textbf {a}}}{{\textbf {b}}\cdot ({\textbf {c}}\times {\textbf {a}})}},\\{\textbf {c}}^{*}&={\frac {2\pi {\textbf {a}}\times {\textbf {b}}}{{\textbf {c}}\cdot ({\textbf {a}}\times {\textbf {b}})}}\end{aligned}}

For an incident electron with wave vector ${\textbf {k}}_{0}=2\pi /\lambda _{0}$ and scattered wave vector ${\begin{aligned}{\textbf {k}}=2\pi /\lambda \end{aligned}}$ , the condition for constructive interference and hence diffraction of scattered electron waves is given by the Laue condition

Figure 4: Ewald's sphere construction for the case of normal incidence of the primary electron beam. The diffracted beams are indexed according to the values of h and l.

{\begin{aligned}{\textbf {k}}-{\textbf {k}}_{0}={\textbf {G}}_{\textrm {hkl}},(1)\end{aligned}}

where (h,k,l) is a set of integers and

{\begin{aligned}{\textbf {G}}_{\textrm {hkl}}=h{\textbf {a}}^{*}+k{\textbf {b}}^{*}+l{\textbf {c}}^{*}\end{aligned}}

is a vector of the reciprocal lattice. The magnitudes of the wave vectors are unchanged, i.e. $|{\textbf {k}}_{0}|=|{\textbf {k}}|$ , since only elastic scattering is considered. Since the mean free path of low energy electrons in a crystal is only a few angstroms, only the first few atomic layers contribute to the diffraction. This means that there are no diffraction conditions in the direction perpendicular to the sample surface. As a consequence the reciprocal lattice of a surface is a 2D lattice with rods extending perpendicular from each lattice point. The rods can be pictured as regions where the reciprocal lattice points are infinitely dense. Therefore, in the case of diffraction from a surface equation (1) reduces to the 2D form:^[2]

{\begin{aligned}{\textbf {k}}^{||}-{\textbf {k}}_{0}^{||}={\textbf {G}}_{\textrm {hk}}=h{\textbf {a}}^{*}+k{\textbf {b}}^{*},(2)\end{aligned}}

where ${\textbf {a}}^{*}$ and ${\textbf {b}}^{*}$ are the primitive translation vectors of the 2D reciprocal lattice of the surface and ${\textbf {k}}^{||},{\textbf {k}}_{0}^{||}$ denote the component of respectively the reflected and incident wave vector parallel to the sample surface. ${\textbf {a}}^{*}$ and ${\textbf {b}}^{*}$ are related to the real space surface lattice in the following way:

{\begin{aligned}{\textbf {a}}^{*}&={\frac {2\pi {\textbf {b}}\times {\hat {\textbf {n}}}}{|{\textbf {a}}\times {\textbf {b}}|}}\\{\textbf {b}}^{*}&={\frac {2\pi {\hat {\textbf {n}}}\times {\textbf {a}}}{|{\textbf {a}}\times {\textbf {b}}|}}\end{aligned}}

The Laue condition equation (2) can readily be visualized using the Ewald's sphere construction. Figure 4 shows a simple illustration of this principle: The wave vector ${\textbf {k}}_{0}$ of the incident electron beam is drawn such that it terminates at a reciprocal lattice point. The Ewald's sphere is then the sphere with radius $|{\textbf {k}}_{0}|$ and origin at the center of the incident wave vector.

By construction, every wave vector centered at the origin and terminating at an intersection between a rod and the sphere will then satisfy the Laue condition and thus represent an allowed diffracted beam.

Interpretation of LEED patterns

Figure 5: Real space- and reciprocal lattices for the case of a) a (100) face of a simple cubic lattice and b) a (2×1) commensurate superstructure. The white spots in the LEED pattern are the extra spots associated with the adsorbate structure.

Figure 4 shows the Ewald's sphere for the case of normal incidence of the primary electron beam, as would be the case in an actual LEED setup. It is apparent that the pattern observed on the fluorescent screen is a direct picture of the reciprocal lattice of the surface. The size of the Ewald's sphere and hence the number of diffraction spots on the screen is controlled by the incident electron energy. From the knowledge of the reciprocal lattice models for the real space lattice can be constructed and the surface can be characterized at least qualitatively in terms of the surface periodicity and the point group. Figure 5.a shows a model of an unreconstructed (100) face of a simple cubic crystal and the expected LEED pattern. The spots are indexed according to the values of h and k.

Superstructures

We now consider the case of an overlaying superstructure on a substrate surface. If the LEED pattern of the underlying (1×1) surface is known, spots due to the superstructure can be identified as extra spots or super spots. Figure 5.b shows the simple example of a (2×1) superstructure on a square lattice.

For a commensurate superstructure the symmetry and the rotational alignment with respect to adsorbent surface can be determined from the LEED pattern. This is easiest shown by using a matrix notation,^[1] where the primitive translation vectors of the superlattice {a_s,b_s} are linked to the primitive translation vectors of the underlying (1x1) lattice {a,b} in the following way

{\begin{aligned}{\textbf {a}}_{s}&=G_{11}{\textbf {a}}+G_{12}{\textbf {b}},\\{\textbf {b}}_{s}&=G_{21}{\textbf {a}}+G_{22}{\textbf {b}}.\end{aligned}}

The matrix for the superstructure then is

{\begin{aligned}G=\left({\begin{array}{cc}G_{11}&G_{12}\\G_{21}&G_{22}\end{array}}\right).\end{aligned}}

Similarly, the primitive translation vectors of the lattice describing the extra spots {a_s^*,b_s^*} are linked to the primitive translation vectors of the reciprocal lattice {a^*,b^*}

{\begin{aligned}{\textbf {a}}_{s}^{*}&=G_{11}^{*}{\textbf {a}}^{*}+G_{12}^{*}{\textbf {b}}^{*},\\{\textbf {b}}_{s}^{*}&=G_{21}^{*}{\textbf {a}}^{*}+G_{22}^{*}{\textbf {b}}^{*}.\end{aligned}}

G^* is related to G in the following way

{\begin{aligned}G^{*}&=(G^{-1})^{T}\\&={\frac {1}{det(G)}}\left({\begin{array}{cc}G_{22}&-G_{21}\\-G_{12}&G_{11}\end{array}}\right).\end{aligned}}

Domains

An essential problem when considering LEED patterns is the existence of symmetrically equivalent domains. Domains may lead to diffraction patterns which have higher symmetry than the actual surface at hand. The reason is that usually the cross sectional area of the primary electron beam (~1 mm²) is large compared to the average domain size on the surface and hence the LEED pattern might be a superposition of diffraction beams from domains oriented along different axes of the substrate lattice.

However, since the average domain size generally is larger than the coherence length of the probing electrons, interference between electrons scattered from different domains can be neglected. Therefore, the total LEED pattern emerges as the incoherent sum of the diffraction patterns associated with the individual domains.

Figure 6 shows the superposition of the diffraction patterns for the two orthogonal domains (2x1) and (1x2) on a square lattice, i.e. for the case where one structure is just rotated by 90° with respect to the other. The (2x1) structure and the respective LEED pattern are shown in figure 5.b. It is apparent that the local symmetry of the surface structure is twofold while the LEED pattern exhibits a fourfold symmetry.

Figure 1 shows a real diffraction pattern of the same situation for the case of a Si(100) surface. However, here the (2x1) structure is formed due to surface reconstruction.

Figure 6: Superposition of the LEED patterns associated with the two orthogonal domains (2x1) and (1x2). The LEED pattern has a fourfold rotational symmetry.

Dynamical theory: multiple scattering

The inspection of the LEED pattern gives a qualitative picture of the surface periodicity i.e. the size of the surface unit cell and to a certain degree of surface symmetries. However it will give no information about the atomic arrangement within a surface unit cell or the sites of adsorbed atoms. For instance if the whole superstructure in figure 5.b is shifted such that the atoms adsorb in bridge sites instead of on-top sites the LEED pattern will be the same.

A more quantitative analysis of LEED experimental data can be achieved by analysis of so-called I-V curves, which are measurements of the intensity versus incident electron energy. The I-V curves can be recorded by using a camera connected to computer controlled data handling or by direct measurement with a movable Faraday cup. The experimental curves are then compared to computer calculations based on the assumption of a particular model system. The model is changed in an iterative process until a satisfactory agreement between experimental and theoretical curves is achieved. A quantitative measure for this agreement is the so-called reliability- or R-factor. A commonly used reliability factor is the one proposed by Pendry.^[6] It is expressed in terms of the logarithmic derivative of the intensity:

{\begin{aligned}L(E)&=I'/I.\end{aligned}}

The R-factor is then given by:

{\begin{aligned}R&=\sum _{g}\int (Y_{\textrm {gth}}-Y_{\textrm {gexpt}})^{2}dE/\sum _{g}\int (Y_{\textrm {gth}}^{2}+Y_{\textrm {gexpt}}^{2})dE,\end{aligned}}

where $Y(E)=L^{-1}/(L^{-2}+V_{oi}^{2})$ and $V_{oi}$ is the imaginary part of the electron self-energy. In general, $R_{p}\leq 0.2$ is considered as a good agreement, $R_{p}\simeq 0.3$ is considered mediocre and $R_{p}\simeq 0.5$ is considered a bad agreement. Figure 7 shows examples of the comparison between experimental I-V spectra and theoretical calculations.

Figure 7: Examples of the comparison between experimental data and a theoretical calculation (an AlNiCo quasicrystal surface). Thanks to R. Diehl and N. Ferralis for providing the data.

Dynamical LEED calculations

The term dynamical stems from the studies of X-ray diffraction and describes the situation where the response of the crystal to an incident wave is included self-consistently and multiple scattering can occur. The aim of any dynamical LEED theory is to calculate the intensities of diffraction of an electron beam impinging on a surface as accurately as possible.

A common method to achieve this is the self-consistent multiple scattering approach.^[7] One essential point in this approach is the assumption that the scattering properties of the surface, i.e. of the individual atoms, are known in detail. The main task then reduces to the determination of the effective wave field incident on the individual scatters present in the surface, where the effective field is the sum of the primary field and the field emitted from all the other atoms. This must be done in a self-consistent way, since the emitted field of an atom depends on the incident effective field upon it. Once the effective field incident on each atom is determined, the total field emitted from all atoms can be found and its asymptotic value far from the crystal then gives the desired intensities.

A common approach in LEED calculations is to describe the scattering potential of the crystal by a "muffin tin" model, where the crystal potential can be imagined being divided up by non-overlapping spheres centered at each atom such that the potential has a spherically symmetric form inside the spheres and is constant everywhere else. The choice of this potential reduces the problem to scattering from spherical potentials, which can be dealt with effectively. The task is then to solve the Schrödinger equation for an incident electron wave in that "muffin tin" potential.

Related Techniques

Tensor LEED

In LEED the exact atomic configuration of a surface is determined by a trial and error process where measured I-V curves are compared to computer-calculated spectra under the assumption of a model structure. From an initial reference structure a set of trial structures is created by varying the model parameters. The parameters are changed until an optimal agreement between theory and experiment is achieved. However, for each trial structure a full LEED calculation with multiple scattering corrections must be conducted. For systems with a large parameter space the need for computational time might become significant. This is the case for complex surfaces structures or when considering large molecules as adsorbates.

Tensor LEED^[8]^[9] is an attempt to reduce the computational effort needed by avoiding full LEED calculations for each trial structure. The scheme is as follows: One first defines a reference surface structure for which the I-V spectrum is calculated. Next a trial structure is created by displacing some of the atoms. If the displacements are small the trial structure can be considered as a small perturbation of the reference structure and first-order perturbation theory can be used to determine the I-V curves of a large set of trial structures.

Spot Profile Analysis Low-Energy Electron Diffraction

A real surface is not perfectly periodic but has many imperfections in the form of dislocations, atomic steps, terraces and the presence of unwanted adsorbed atoms. This departure from a perfect surface leads to a broadening of the diffraction spots and adds to the background intensity in the LEED pattern.

SPA-LEED^[10] is a technique where the intensity of diffraction beams is measured in order to determine the diffraction spot profiles. The spots are sensitive to the irregularities in the surface structure and their examination therefore permits more-detailed conclusions about some surface characteristics. Using SPA-LEED may for instance permit a quantitative determination of the surface roughness, terrace sizes or surface steps.^[10]

Other

Spin-Polarized Low Energy Electron Diffraction
Inelastic Low Energy Electron Diffraction
Very Low Energy Electron Diffraction
Reflection high-energy electron diffraction

References

1 2 3 K. Oura; V.G. Lifshifts; A.A. Saranin; A. V. Zotov; M. Katayama (2003). Surface Science. Springer-Verlag, Berlin Heidelberg New York. pp. 1–45.
1 2 3 M.A. Van Hove; W.H. Weinberg; C. M. Chan (1986). Low-Energy Electron Diffraction. Springer-Verlag, Berlin Heidelberg New York. pp. 1–27, 46–89, 92–124, 145–172. ISBN 3-540-16262-3. doi:10.1002/maco.19870380711.
↑ Zangwill, A., "Physics at Surfaces", Cambridge University Press (1988), p.33
↑ Pendry (1974). Low-Energy Electron Diffraction. Academic Press Inc. (London) LTD. pp. 1–75.
↑ C. Kittel (1996). "2". Introduction to Solid State Physics. John Wiley, US.
↑ J.B. Pendry (1980). "Reliability Factors for LEED Calculations". J. Phys. C. 13: 937. Bibcode:1980JPhC...13..937P. doi:10.1088/0022-3719/13/5/024.
↑ E.G. McRae (1967). "Self-Consistent Multiple-Scattering Approach to the Interpretation of Low-Energy Electron Diffraction". Surface Science. 8 (1-2): 14–34. Bibcode:1967SurSc...8...14M. doi:10.1016/0039-6028(67)90071-4.
↑ P.J. Rous J.B. Pendry (1989). "Tensor LEED I: A Technique for high speed surface structure determination by low energy electron diffraction.". Comp. Phys. Comm. 54 (1): 137–156. Bibcode:1989CoPhC..54..137R. doi:10.1016/0010-4655(89)90039-8.
↑ P.J. Rous J.B. Pendry (1989). "The theory of Tensor LEED.". Surf. Sci. 219 (3): 355–372. Bibcode:1989SurSc.219..355R. doi:10.1016/0039-6028(89)90513-X.
1 2 M. Henzler (1982). "Studies of Surface Imperfections". Appl. Surf. Sci. 11/12: 450. Bibcode:1982ApSS...11..450H. doi:10.1016/0378-5963(82)90092-7.

P. Goodman (General Editor), Fifty Years of Electron Diffraction, D. Reidel Publishing, 1981
D. Human et al., Low energy electron diffraction using an electronic delay-line detector, Rev. Sci. Inst. 77 023302 (2006)

External links

LEED programm packages

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