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132-S-100 - Avaya Sales Certification Specialist - Dump Information

Vendor : Avaya
Exam Code : 132-S-100
Exam Name : Avaya Sales Certification Specialist
Questions and Answers : 49 Q & A
Updated On : February 23, 2018
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132-S-100 Questions and Answers

132-S-100


  1. Areas where we cannot affect business processes

  2. Avaya's key strengths in CEBP

  3. Cisco's SONA software

  4. Part of BEA's MicroServices Architecture


Answer: B


QUESTION: 43

What type of enterprise is the Avaya Distributed Office solution perfect for?


  1. Medium-sized enterprises that have growth potential

  2. Large enterprises with multiple branches

  3. Small enterprises with a few remote workers

  4. Distributed Office is built to fit any enterprise


Answer: B


QUESTION: 44

The Avaya "Flatten, Consolidate and Extend" value proposition means .


  1. Deploying separate stand-alone communications systems in every location across the enterprise

  2. Investing more heavily in the infrastructure

  3. Addressing only telephony applications, but handling contact centers separately

  4. Moving from a group of loosely connected standalone systems to a centralized application approach


Answer: D


QUESTION: 45

What is a key Unified Communications value message for a "Road Warrior" type of worker?


  1. Making the mobile device an extension of the deskphone


  2. Control of telephony

  3. Intuitive interfaces allowing a seamless shift between locations

  4. Use of dual-connect phone


Answer: A


QUESTION: 46

Which two Avaya solutions should you use when customers find employees unreachable or unproductive at the office and have IT departments having increasing difficulty controlling mobility, spending, and usage? (Choose two.)


  1. Embed mobility applications into core IP Telephony software.

  2. Provide cell phones to each mobile employee

  3. Extend customer announcements, voicemail greetings, and other applications.

  4. Utilize speech access to satisfy the individual's requirements


Answer: A, C


QUESTION: 47

Which is NOT a top business imperative in the IPT marketplace?


  1. Managing and maintaining multiple, non-integrated systems

  2. Needing consistent service/delivery at branch or remote locations

  3. Needing advanced communications tools to compete effectively

  4. Implementing the latest new technology


Answer: D


QUESTION: 48

Unified Communications solutions represent of Avaya's estimated addressable market


  1. 15%

  2. 27%


  3. 33%

  4. 41%


Answer: D


QUESTION: 49

Which section of the Solution Messaging Card is best described by where Avaya lists specific details and how a problem manifests itself at the individual level?


  1. Solution linkage

  2. Business impact

  3. Trend relevance

  4. Potential pains

  5. Metrics proof of value


Answer: D


Avaya 132-S-100 Exam (Avaya Sales Certification Specialist) Detailed Information

Credentials & Certifications
Sharpen Your Technical Skills—Get Certified on Avaya Solutions
Professional Credentials and Technical Certifications
For every level of knowledge and expertise, Avaya certification programs can enhance your ability to effectively deploy and use Avaya communications applications and technology.
Programs are available by area of focus and for different skill levels. Courses include rigorous study and hands-on learning, complimented by a blend of online tests and proctored exams to validate your competencies. Certifications require passing scores on all examinations.
Maintain Your Market Edge
The skills and knowledge you demonstrate through certification can help you make an immediate impact on current projects. Plus, you gain resume-worthy, career-building skills. You’ll be better able to sell, design, implement and maintain Avaya Solutions while teaching others new skills along the way. Certification shows you are motivated, experienced, and committed to achieve excellence in your field. Avaya Professional Credentials and Certifications are recognized across the globe.
The Avaya Professional Credential Program is designed to ensure individuals have the knowledge and skills to successfully sell, design, implement, and maintain Avaya products and solutions that exceed customer expectations.
The Avaya Professional Credential Program consists of Sales, Design and Support Credentials and distinguishes between Solution Credentials and Product specific Credentials.
To learn more about the Program select the individual graphics above or the workbook tabs.
Avaya Professional Credentials and Certifications
The Avaya Professional Credential Program consists of Sales and Services Credentials, and uses a blend of Online Tests and Proctored Exams to validate competencies. Refer to the Avaya Professional Credential Program Overview for details.
In support of the credential program, Avaya Learning offers a wide variety of training content to meet the needs of our Partners, Customers, and Associates.
Fundamental to all Avaya Professional Credentials is a solid understanding of the core technologies upon which the products and solutions are built. Avaya recommends the programs of leading industry players to provide foundational knowledge: WestNet Learning (Foundational Technology Expert) and The SIP School (SSCA).
Avaya Professional Credential Program
Note: Some credentials are available only to Avaya Partners and Avaya Associates. Please
read the following credential descriptions to confirm eligibility.
The Avaya Professional Credential Program is designed to ensure individuals have the knowledge and
skills to successfully sell, design, implement and maintain Avaya products and solutions that exceed
customer expectations. The Avaya Professional Credential Program currently consists of Sales,
Design, and Services Credentials and distinguishes between Solution Credentials and Product
Specific Credentials.
Sales & Design Credentials
Avaya Engagement Solutions Certifications
Services Credentials
Avaya Engagement Solutions Certifications
ACDS - Avaya Certified Design Specialist
ACSP - Avaya Certified Sales Professional
Avaya Product Professional Credentials
APDS - Avaya Professional Design Specialist
APSS - Avaya Professional Sales Specialist
ACSS - Avaya Certified Solution Specialist
ACIS - Avaya Certified Integration Specialist
Avaya Product Certifications
ACSS - Avaya Certified Support Specialist
ACIS - Avaya Certified Implementation Specialist
Avaya Product Professional Credentials
ASPS - Avaya Support Professional Specialist
AIPS - Avaya Implementation Professional Specialist
Avaya uses a blend of Online Tests and Proctored Exams to validate competencies. Professional Specialist
credentials are awarded based upon passing Online Tests. Certified credentials incorporate Proctored Exams
and Online Tests as a requirement to earn the credential.
For a complete listing of Avaya credentials by product / solution area, please visit the Avaya Professional Credential
Program page on the Avaya Learning Center at www.avaya-learning.com.
Fundamental to all Avaya Professional Credentials is a solid understanding of the core technologies
03 October 2016 v1 3
upon which the products and solutions are built. Avaya recommends the programs of leading industry players
to provide foundational knowledge: WestNet Learning (Foundational Technology Expert) and The SIP School
(SSCA).
In support of the Credential Program, Avaya Learning offers a wide variety of training content to meet the
needs of our Partners, Customers, and Associates.
Avaya Professional Sales Specialist (APSS)
APSS validates a candidate has a basic-to-intermediary level of knowledge to sell Avaya products and customer focused
solutions.
An Avaya Professional Sales Specialist understands the competitive global landscape, evaluating customer needs,
identifying and recommending the right Avaya solution and communicating its business value.
APSS Credentials use online tests, are valid for 2 years and are reserved exclusively for Avaya Channel Partners and
Associates.
Exception: APSS – Avaya Aura® Application Server 5300 (APSS -1101) remains a one year credential until
further notice.
Avaya Professional Design Specialist (APDS)
APDS validates a candidate has an introductory level of technical proficiency necessary to create specific
designs and build foundational knowledge for solution designs based on the customer requirements.
The Avaya Professional Design Specialist has the skills and knowledge necessary to review a customer’s
current configuration, understand their future needs and design an Avaya solution for today and tomorrow. The
Design Specialist creates architectural designs and migration strategies ensuring both integration to current
networks and future readiness of customer communication solutions.
APDS Credentials use online tests, are valid for 2 years and are reserved exclusively for Avaya Channel
Partners and Associates.
Avaya Certified Sales Professional (ACSP) In planning
ACSP validates that the candidate has achieved an advanced understanding of and competence in Avaya
Sales skills and processes for sales strategy and deployment.
Avaya Certified Sales Professional (ACSP) curriculum for Avaya Engagement Solutions captures both the
Avaya Sales approach and the Engagement Solutions for both Avaya Associates and Business Partners.
Building upon the foundation established with the Avaya Professional Sales Specialist (APSS) curriculum,
students completing the ACSP curriculum will be able to sell and position solutions that address the
customer’s issues and objectives.
ACSP Credentials use proctored exams, are valid for 2 years and are reserved exclusively for Avaya Channel
Partners and Associates.
Note: The ACSP credentials are currently being planned and not fully released.
03 October 2016 v1 4
Avaya Certified Design Specialist (ACDS)
ACDS validates that the candidate has an intermediary level of technical proficiency necessary to
create specific greenfield, upgrade and migration solution designs based on the customer business
needs.
Avaya recognizes that individuals responsible for designing customer solutions demonstrate
advanced Sales Engineering skills and therefore should be distinguished with a credential that
signifies their achievement.
ACDS Credentials use proctored exams and online tests, are valid for 2 years and are reserved
exclusively for Avaya Channel Partners and Associates.
Note: The ACDS portfolio has undergone a major redesign to provide the Avaya Sales Engineer
(SE) community a growth path to mastery in Avaya Engagement Solutions. The ACDS curriculum
for Avaya Engagement Solutions instills a common methodology and approach to solution design
across the entire SE community and builds upon the foundation established with the Avaya
Professional Design Specialist (APDS) curriculum.
Avaya Implementation Professional Specialist (AIPS)
AIPS validates a candidate has achieved an enhanced level of proficiency focused on installing,
configuring, and troubleshooting a specified Avaya product or product family.
The Avaya Implementation Professional Specialist can implement, validate and troubleshoot the
installation of a single product, single system or product family. The Implementation Specialist installs
hardware and software, configures the solution, performs initial administration and acceptance testing
to diagnose and correct installation issues.
AIPS Credentials use online tests, are valid for 2 years and are open to all audiences.
Avaya Support Professional Specialist (ASPS)
ASPS validates a candidate has achieved an advanced understanding of and competence in
troubleshooting, maintaining and administration of Avaya industry leading communications products.
The Avaya Support Professional Specialist gathers and interprets system data, identifies issues and
makes changes to ensure maximum availability and performance of a customer’s network. The
Support Specialist uses their advanced Avaya troubleshooting, maintenance and administration
capabilities to efficiently and accurately resolve customer’s communication issues.
ASPS Credentials use online tests, are valid for 2 years and are open to all audiences.
03 October 2016 v1 5
Avaya Certified Implementation Specialist (ACIS)
ACIS certifies a candidate has achieved an enhanced level of proficiency focused on installing, configuring, and
troubleshooting a specified Avaya product or product family.
The Avaya Certified Implementation Specialist can implement, validate and troubleshoot the installation of a single product,
single system or product family. The Implementation Specialist installs hardware and software, configures the solution,
performs initial administration and acceptance testing to diagnose and correct installation issues.
ACIS Certifications use proctored exams, are valid for 2 years and are open to all audiences.
Avaya Certified Support Specialist (ACSS)
ACSS certifies a candidate has achieved an advanced understanding of and competence in troubleshooting,
maintaining and administration of Avaya industry leading communications products.
The Avaya Certified Support Specialist gathers and interprets system data, identifies issues and makes changes to
ensure maximum availability and performance of a customer’s network. The Support Specialist uses their advanced
Avaya troubleshooting, maintenance and administration capabilities to efficiently and accurately resolve customer’s
communication issues.
ACSS Certifications use proctored exams, are valid for 2 years and are open to all audiences.
Avaya Certified Integration Specialist (ACIS)
ACIS certifies a candidate has achieved a level of proficiency required to integrate and implement core and complex
solutions based on reference architectures from Avaya customer scenarios.
The Avaya Certified Integration Specialist demonstrates the integration of enterprise architecture solutions in order
to install, validate, and troubleshoot the implementation. The Integration Specialist holds a technical ability at a level
that ensures the successful integration, configuration, and support of the solution reference architectures.
ACIS Certifications use proctored exams and online tests, are valid for 2 years and are open to all audiences.
Avaya Certified Solution Specialist (ACSS)
ACSS certifies a candidate has achieved an intermediate - advanced level of proficiency required to diagnose,
isolate and support multi products within Avaya solution architecture.
The Avaya Certified Solution Specialist comprehends the methodology to isolate and diagnose single and multiple
problems within the enterprise solution architectures, technologies and protocols. The Solution Specialist holds a
technical ability at a level that ensures the successful maintenance, and support of solution architecture.
ACSS Certifications use proctored exams and online tests, are valid for 2 years and are open to all audiences.
To obtain an ACSS credential individuals need to hold the relevant ACIS credential.
03 October 2016 v1 6
Questions?
About Avaya Learning
Avaya Learning develops and delivers industry leading training for Avaya products and solutions. Avaya Learning
specifically focuses on Avaya’s product launches, sales force and channel enablement - including solution and
executive selling, skills development and certification. Avaya Learning uses a blended learning approach offering a
combination of self-paced, virtual interactive and classroom learning environments to maximize effectiveness and
decrease time required to reach proficiency.
Avaya Learning supports and maintains the Avaya Learning Center where both course details and information on the
Avaya Professional Credential Program can be found

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    Stretched-coordinate PMLs for Maxwell’s equations within the discontinuous Galerkin time-domain formula

    M. okönig, ok. Busch, and J. Niegemann, “The discontinuous Galerkin time-area components for Maxwell’s equations with anisotropic materials,” Photonics Nanostruct. Fundam. Appl. eight, 303–309 (2010).[Crossref]

    A. Hille, R. Kullock, S. Grafström, and L. M. Eng, “improving nano-optical simulations through curved elements carried out within the discontinuous Galerkin formulation computational,” J. Comput. Theor. Nanosci. 7, 1581–1586 (2010).[Crossref]

    N. Feth, M. okayönig, M. Husnik, ok. Stannigel, J. Niegemann, okay. Busch, M. Wegener, and S. Linden, “Electromagnetic interplay of cut up-ring resonators: the position of separation and relative orientation,” choose. specific 18, 6545–6554 (2010).[Crossref] [PubMed]

    R. Diehl, k. Busch, and J. Niegemann, “assessment of low-storage Runge-Kutta schemes for discontinuous Galerkin time-area simulations of Maxwell’s equations,” J. Comput. Theor. Nanosci. 7, 1572–1580 (2010).[Crossref]

    J. Niegemann, M. könig, ok. Stannigel, and ok. Busch, “better-order time-domain strategies for the analysis of nano-photonic techniques,” Photonics Nanostruct. Fundam. Appl. 7, 2–11 (2009).[Crossref]

    J. Niegemann, W. Pernice, and okay. Busch, “Simulation of optical resonators the usage of DGTD and FDTD,” J. decide. A: Pure Appl. opt. eleven, 114015 (2009).[Crossref]

    T. Hagstrom and S. Lau, “Radiation boundary conditions for Maxwell’s equations: A evaluate of correct time-domain formulations,” J. Comput. Math. 25, 305–336 (2007).

    T. Lu, P. Zhang, and W. Cai, “Discontinuous Galerkin strategies for dispersive and lossy Maxwell’s equations and PML boundary situations,” J. Comput. Phys. 200, 549–580 (2004).[Crossref]

    J. S. Hesthaven and T. Warburton, “Nodal excessive-order methods on unstructured grids–I. Time-area answer of Maxwell’s equations,” J. Comput. Phys. 181, 186–221 (2002).[Crossref]

    Z. S. Sacks, D. M. Kingsland, R. Lee, and J.-F. Lee, “a wonderfully matched anisotropic absorber for use as an absorbing boundary situation,” IEEE Trans. Antennas Propag. forty three, 1460–1463 (1995).[Crossref]

    W. C. bite and W. H. Weedon, “A 3D completely matched medium from modified maxwell’s equations with stretched coordinates,” Microwave opt. Technol. Lett. 7, 599–604 (1994).[Crossref]

    M. H. chippie and C. A. Kennedy, “Fourth-order 2N-storage Runge–Kutta schemes,” NASA Tech. Memo. 109112 (1994).

    J. P. Bérenger, “a wonderfully matched layer for the absorption of electromagnetic waves,” J. Comput. Phys. 114, 185–200 (1994).[Crossref]

    J. P. Bérenger, “a wonderfully matched layer for the absorption of electromagnetic waves,” J. Comput. Phys. 114, 185–200 (1994).[Crossref]

    J.-P. Bérenger, perfectly Matched Layer (PML) for Computational Electromagnetics (Morgan & Claypool Publishers, 2007).

    R. Diehl, ok. Busch, and J. Niegemann, “evaluation of low-storage Runge-Kutta schemes for discontinuous Galerkin time-domain simulations of Maxwell’s equations,” J. Comput. Theor. Nanosci. 7, 1572–1580 (2010).[Crossref]

    N. Feth, M. könig, M. Husnik, k. Stannigel, J. Niegemann, okay. Busch, M. Wegener, and S. Linden, “Electromagnetic interplay of break up-ring resonators: the role of separation and relative orientation,” decide. categorical 18, 6545–6554 (2010).[Crossref] [PubMed]

    M. könig, k. Busch, and J. Niegemann, “The discontinuous Galerkin time-domain formulation for Maxwell’s equations with anisotropic materials,” Photonics Nanostruct. Fundam. Appl. eight, 303–309 (2010).[Crossref]

    J. Niegemann, M. könig, okay. Stannigel, and okay. Busch, “bigger-order time-area methods for the analysis of nano-photonic techniques,” Photonics Nanostruct. Fundam. Appl. 7, 2–eleven (2009).[Crossref]

    J. Niegemann, W. Pernice, and ok. Busch, “Simulation of optical resonators the usage of DGTD and FDTD,” J. decide. A: Pure Appl. opt. 11, 114015 (2009).[Crossref]

    T. Lu, P. Zhang, and W. Cai, “Discontinuous Galerkin strategies for dispersive and lossy Maxwell’s equations and PML boundary situations,” J. Comput. Phys. 200, 549–580 (2004).[Crossref]

    M. H. wood worker and C. A. Kennedy, “Fourth-order 2N-storage Runge–Kutta schemes,” NASA Tech. Memo. 109112 (1994).

    W. C. chunk and W. H. Weedon, “A 3D completely matched medium from modified maxwell’s equations with stretched coordinates,” Microwave decide. Technol. Lett. 7, 599–604 (1994).[Crossref]

    R. Diehl, k. Busch, and J. Niegemann, “assessment of low-storage Runge-Kutta schemes for discontinuous Galerkin time-domain simulations of Maxwell’s equations,” J. Comput. Theor. Nanosci. 7, 1572–1580 (2010).[Crossref]

    A. Hille, R. Kullock, S. Grafström, and L. M. Eng, “improving nano-optical simulations through curved features applied inside the discontinuous Galerkin components computational,” J. Comput. Theor. Nanosci. 7, 1581–1586 (2010).[Crossref]

    N. Feth, M. könig, M. Husnik, ok. Stannigel, J. Niegemann, ok. Busch, M. Wegener, and S. Linden, “Electromagnetic interplay of split-ring resonators: the position of separation and relative orientation,” choose. specific 18, 6545–6554 (2010).[Crossref] [PubMed]

    A. Hille, R. Kullock, S. Grafström, and L. M. Eng, “improving nano-optical simulations through curved facets carried out inside the discontinuous Galerkin system computational,” J. Comput. Theor. Nanosci. 7, 1581–1586 (2010).[Crossref]

    A. Taflove and S. C. Hagness, Computational Electrodynamics: The Finite-difference Time-area components, 3rd ed. (Artech apartment, 2005).

    T. Hagstrom and S. Lau, “Radiation boundary situations for Maxwell’s equations: A evaluation of accurate time-domain formulations,” J. Comput. Math. 25, 305–336 (2007).

    J. S. Hesthaven and T. Warburton, “Nodal excessive-order strategies on unstructured grids–I. Time-domain solution of Maxwell’s equations,” J. Comput. Phys. 181, 186–221 (2002).[Crossref]

    J. S. Hesthaven and T. Warburton, Nodal Discontinuous Galerkin strategies—Algorithms, evaluation, and purposes (Springer, 2007).[PubMed]

    A. Hille, R. Kullock, S. Grafström, and L. M. Eng, “improving nano-optical simulations through curved elements carried out inside the discontinuous Galerkin components computational,” J. Comput. Theor. Nanosci. 7, 1581–1586 (2010).[Crossref]

    N. Feth, M. okönig, M. Husnik, okay. Stannigel, J. Niegemann, k. Busch, M. Wegener, and S. Linden, “Electromagnetic interaction of cut up-ring resonators: the position of separation and relative orientation,” choose. express 18, 6545–6554 (2010).[Crossref] [PubMed]

    M. H. wood worker and C. A. Kennedy, “Fourth-order 2N-storage Runge–Kutta schemes,” NASA Tech. Memo. 109112 (1994).

    Z. S. Sacks, D. M. Kingsland, R. Lee, and J.-F. Lee, “a superbly matched anisotropic absorber to be used as an absorbing boundary circumstance,” IEEE Trans. Antennas Propag. 43, 1460–1463 (1995).[Crossref]

    N. Feth, M. okönig, M. Husnik, okay. Stannigel, J. Niegemann, k. Busch, M. Wegener, and S. Linden, “Electromagnetic interplay of break up-ring resonators: the role of separation and relative orientation,” choose. specific 18, 6545–6554 (2010).[Crossref] [PubMed]

    M. könig, okay. Busch, and J. Niegemann, “The discontinuous Galerkin time-domain system for Maxwell’s equations with anisotropic materials,” Photonics Nanostruct. Fundam. Appl. eight, 303–309 (2010).[Crossref]

    J. Niegemann, M. könig, okay. Stannigel, and okay. Busch, “greater-order time-domain methods for the analysis of nano-photonic methods,” Photonics Nanostruct. Fundam. Appl. 7, 2–eleven (2009).[Crossref]

    A. Hille, R. Kullock, S. Grafström, and L. M. Eng, “improving nano-optical simulations via curved facets carried out inside the discontinuous Galerkin system computational,” J. Comput. Theor. Nanosci. 7, 1581–1586 (2010).[Crossref]

    T. Hagstrom and S. Lau, “Radiation boundary conditions for Maxwell’s equations: A assessment of correct time-area formulations,” J. Comput. Math. 25, 305–336 (2007).

    Z. S. Sacks, D. M. Kingsland, R. Lee, and J.-F. Lee, “a superbly matched anisotropic absorber for use as an absorbing boundary condition,” IEEE Trans. Antennas Propag. 43, 1460–1463 (1995).[Crossref]

    Z. S. Sacks, D. M. Kingsland, R. Lee, and J.-F. Lee, “a superbly matched anisotropic absorber for use as an absorbing boundary circumstance,” IEEE Trans. Antennas Propag. 43, 1460–1463 (1995).[Crossref]

    R. J. LeVeque, Finite quantity methods for Hyperbolic complications (Cambridge tuition Press, 2002).[Crossref]

    N. Feth, M. könig, M. Husnik, k. Stannigel, J. Niegemann, ok. Busch, M. Wegener, and S. Linden, “Electromagnetic interaction of break up-ring resonators: the function of separation and relative orientation,” decide. specific 18, 6545–6554 (2010).[Crossref] [PubMed]

    T. Lu, P. Zhang, and W. Cai, “Discontinuous Galerkin strategies for dispersive and lossy Maxwell’s equations and PML boundary situations,” J. Comput. Phys. 200, 549–580 (2004).[Crossref]

    P. Monk, Finite element strategies for Maxwell’s Equations (Oxford tuition Press, 2003).[Crossref] [PubMed]

    N. Feth, M. okayönig, M. Husnik, ok. Stannigel, J. Niegemann, k. Busch, M. Wegener, and S. Linden, “Electromagnetic interplay of break up-ring resonators: the position of separation and relative orientation,” decide. express 18, 6545–6554 (2010).[Crossref] [PubMed]

    R. Diehl, ok. Busch, and J. Niegemann, “assessment of low-storage Runge-Kutta schemes for discontinuous Galerkin time-domain simulations of Maxwell’s equations,” J. Comput. Theor. Nanosci. 7, 1572–1580 (2010).[Crossref]

    M. okönig, okay. Busch, and J. Niegemann, “The discontinuous Galerkin time-domain formulation for Maxwell’s equations with anisotropic substances,” Photonics Nanostruct. Fundam. Appl. eight, 303–309 (2010).[Crossref]

    J. Niegemann, M. okönig, ok. Stannigel, and k. Busch, “greater-order time-domain methods for the analysis of nano-photonic programs,” Photonics Nanostruct. Fundam. Appl. 7, 2–11 (2009).[Crossref]

    J. Niegemann, W. Pernice, and okay. Busch, “Simulation of optical resonators the use of DGTD and FDTD,” J. opt. A: Pure Appl. choose. eleven, 114015 (2009).[Crossref]

    J. Niegemann, W. Pernice, and k. Busch, “Simulation of optical resonators the usage of DGTD and FDTD,” J. choose. A: Pure Appl. choose. eleven, 114015 (2009).[Crossref]

    Z. S. Sacks, D. M. Kingsland, R. Lee, and J.-F. Lee, “a wonderfully matched anisotropic absorber to be used as an absorbing boundary situation,” IEEE Trans. Antennas Propag. 43, 1460–1463 (1995).[Crossref]

    N. Feth, M. okönig, M. Husnik, ok. Stannigel, J. Niegemann, ok. Busch, M. Wegener, and S. Linden, “Electromagnetic interaction of cut up-ring resonators: the position of separation and relative orientation,” decide. express 18, 6545–6554 (2010).[Crossref] [PubMed]

    J. Niegemann, M. könig, okay. Stannigel, and ok. Busch, “higher-order time-domain methods for the evaluation of nano-photonic systems,” Photonics Nanostruct. Fundam. Appl. 7, 2–11 (2009).[Crossref]

    A. Taflove and S. C. Hagness, Computational Electrodynamics: The Finite-change Time-area method, 3rd ed. (Artech apartment, 2005).

    J. S. Hesthaven and T. Warburton, “Nodal high-order methods on unstructured grids–I. Time-area answer of Maxwell’s equations,” J. Comput. Phys. 181, 186–221 (2002).[Crossref]

    J. S. Hesthaven and T. Warburton, Nodal Discontinuous Galerkin methods—Algorithms, evaluation, and applications (Springer, 2007).[PubMed]

    W. C. bite and W. H. Weedon, “A 3D perfectly matched medium from modified maxwell’s equations with stretched coordinates,” Microwave decide. Technol. Lett. 7, 599–604 (1994).[Crossref]

    N. Feth, M. könig, M. Husnik, ok. Stannigel, J. Niegemann, ok. Busch, M. Wegener, and S. Linden, “Electromagnetic interaction of cut up-ring resonators: the position of separation and relative orientation,” decide. specific 18, 6545–6554 (2010).[Crossref] [PubMed]

    T. Lu, P. Zhang, and W. Cai, “Discontinuous Galerkin methods for dispersive and lossy Maxwell’s equations and PML boundary circumstances,” J. Comput. Phys. 200, 549–580 (2004).[Crossref]

    Z. S. Sacks, D. M. Kingsland, R. Lee, and J.-F. Lee, “a wonderfully matched anisotropic absorber for use as an absorbing boundary condition,” IEEE Trans. Antennas Propag. 43, 1460–1463 (1995).[Crossref]

    T. Hagstrom and S. Lau, “Radiation boundary conditions for Maxwell’s equations: A assessment of accurate time-area formulations,” J. Comput. Math. 25, 305–336 (2007).

    J. P. Bérenger, “a superbly matched layer for the absorption of electromagnetic waves,” J. Comput. Phys. 114, 185–200 (1994).[Crossref]

    J. S. Hesthaven and T. Warburton, “Nodal high-order strategies on unstructured grids–I. Time-area solution of Maxwell’s equations,” J. Comput. Phys. 181, 186–221 (2002).[Crossref]

    T. Lu, P. Zhang, and W. Cai, “Discontinuous Galerkin methods for dispersive and lossy Maxwell’s equations and PML boundary conditions,” J. Comput. Phys. 200, 549–580 (2004).[Crossref]

    A. Hille, R. Kullock, S. Grafström, and L. M. Eng, “enhancing nano-optical simulations via curved points applied in the discontinuous Galerkin formulation computational,” J. Comput. Theor. Nanosci. 7, 1581–1586 (2010).[Crossref]

    R. Diehl, okay. Busch, and J. Niegemann, “comparison of low-storage Runge-Kutta schemes for discontinuous Galerkin time-area simulations of Maxwell’s equations,” J. Comput. Theor. Nanosci. 7, 1572–1580 (2010).[Crossref]

    J. Niegemann, W. Pernice, and ok. Busch, “Simulation of optical resonators the use of DGTD and FDTD,” J. opt. A: Pure Appl. decide. eleven, 114015 (2009).[Crossref]

    W. C. chew and W. H. Weedon, “A 3D perfectly matched medium from modified maxwell’s equations with stretched coordinates,” Microwave decide. Technol. Lett. 7, 599–604 (1994).[Crossref]

    M. H. wood worker and C. A. Kennedy, “Fourth-order 2N-storage Runge–Kutta schemes,” NASA Tech. Memo. 109112 (1994).

    N. Feth, M. okayönig, M. Husnik, ok. Stannigel, J. Niegemann, k. Busch, M. Wegener, and S. Linden, “Electromagnetic interplay of split-ring resonators: the function of separation and relative orientation,” decide. categorical 18, 6545–6554 (2010).[Crossref] [PubMed]

    J. Niegemann, M. könig, ok. Stannigel, and ok. Busch, “better-order time-domain strategies for the analysis of nano-photonic systems,” Photonics Nanostruct. Fundam. Appl. 7, 2–eleven (2009).[Crossref]

    M. könig, ok. Busch, and J. Niegemann, “The discontinuous Galerkin time-area method for Maxwell’s equations with anisotropic materials,” Photonics Nanostruct. Fundam. Appl. eight, 303–309 (2010).[Crossref]

    J. S. Hesthaven and T. Warburton, Nodal Discontinuous Galerkin methods—Algorithms, analysis, and functions (Springer, 2007).[PubMed]

    A. Taflove and S. C. Hagness, Computational Electrodynamics: The Finite-change Time-domain formula, third ed. (Artech residence, 2005).

    J.-P. Bérenger, completely Matched Layer (PML) for Computational Electromagnetics (Morgan & Claypool Publishers, 2007).

    P. Monk, Finite element strategies for Maxwell’s Equations (Oxford institution Press, 2003).[Crossref] [PubMed]

    R. J. LeVeque, Finite volume methods for Hyperbolic issues (Cambridge college Press, 2002).[Crossref]




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