• No se han encontrado resultados

CMAM

N/A
N/A
Protected

Academic year: 2024

Share "CMAM"

Copied!
23
0
0

Texto completo

(1)

The CMAM “Centro de Micro

Análisis de Materiales” and its facilities

presented by Alessandro Zucchiatti

European Network of Small Accelerator Facilities ENSAF Sevilla Workshop 19-21 October 2016

CMAM

(2)

The UAM and CMAM

UAM

Mailing Address

Centro de Micro-Análisis de Materiales Calle de Faraday 3,

Universidad Autónoma de Madrid Campus de Cantoblanco

E-28049, Madrid, Spain Phone number

(+34) 91 497 3621 (Switchboard) Email Address

[email protected] WEB page

http://www.cmam.uam.es

UAM

CMAM

(3)

The UAM numbers

Students: 32,345​ 23,000

Undergraduate

9,345 Postgraduate ​

Academic staff: 2,791

Administrative staff:

987

Yearly Budget 2016: 263.3 M€

RANKING 2016 POSITION

Top 200 QS World 210th Global, 93rd Europe, 3rd Spain

University Rankings Physics and Astronomy 51-100 Global

US news best global 209th Global, 87th Europe, 3rd Spain

universities Physics 53th Global, 19th Europe, 1stSpain

Shanghai (ARWU) 201-300 Global 2-3rd Spain 51-75: Mathematics (2015) 51-75: Physics (2015)

200: Chemistry (2015) 9th Global 3rd EU 1st Spain

(4)

UAM research excellence

Four advanced research “platforms”

• Nanoscience and Advanced Materials

41 groups located at or near the UAM+CSIC Campus. 9 of the 20 most relevant condensed matter physicists in Spain (H index above 32). Six research centres

• Biology and Biomedicine

• Theoretical Physics and Mathematics

• Social and Human Sciences

CMAM

(5)

CMAM Research

Archaeometry

Photonics

Biophysics

Solid State Physics

Energy Related Materials

Nuclear Physics Surface Physics

Ion-Solid Interactions

Micro-patterning

Publications

Citations

H=27

(6)

CMAM numbers

Actual staff: 24

• 10 scientists,

• 1 PhD student,

• 9 technicians,

• 4 administrative

Past Staff of CMAM: 57

Total Investment: 11.35 M€

Annual cost (including technical staff): 730 k€

Staff: 60%

Research: 23%

Services: 17%

Annual cost (including all staff): 1.09 M€

Doctoral Theses: 13 Master and Erasmus

students: 36 High school students: 144

(7)

CMAM numbers

Publications Citations

H=27

Ions produced

(8)

Infrastructures: 5MV accelerator

• Co-axial Cockroft-Walton

• Tandem

• Very low ripple <50V @ 5MV

2 ion sources:

Duoplasmatron

Sputtering

Project begins 1998

Earthbreaking 1999

Accelerator installed 09/2002

Inaugurated 23/03/2003

(9)

Infrastructure: Ancillary Labs

Optics

Chemistry & sample prep. Electronics Workshop

Mechanics Workshop Microscopy

Sputtering

Software & networking … plus the UAM services on campus: SIDI, SEGAINVEX,TI

(10)

Beamlines

• Standard

• External micro-beam

• ERDA-ToF (3 experimental stations)

• Nuclear Physics

• Internal micro-beam

• Nuclear Reaction Analysis

• Implantation

NRA

(11)

Standard beamline

• IBA techniques (RBS,RBSc,ERDA,NRA,PIXE)

• IBMM over small areas

• 4 axis goniometer (0.01 deg)

• Two particle detectors (fixed & movable).

• A high sensitivity optical camera

• A special viewport for far-infrared (thermal) camera

• A few ports are available for PIGE and IBIL when necessary.

• Faraday Cup associated to target holder

• Ions up to Br regularly used in STD

• Very versatile

growth of wurzite-CdZnO single phase

(12)

Internal micro-beam

PIXE, RBS and STIM

• Micrometric resolution

• Ion-energy combination up to Cl

• RBS detector can be used for relative

charge measurement

• Beam scan 500x500 microns

• Mainly for Biological materials and to

irradiate over micropatterns

(13)

Implantation line

Isolated chamber acts as FC

• Min. beam size 2mm + 4”x4” scans

• Ions up to Au2 -170<Ttarget<600

• Instruments additions (e.g.

elipsometry)

• New fs-laser+ion double irradiation (in progress)

• Beam degrader for a “white” spectrum (CIEMAT ready to mount)

•Used mainly to irradiate Energy related and optical materials

(14)

External micro-beam

• FWHM res. 20-50 µm @3mm

• 2 X-ray detectors for PIXE

• 1 silicon implanted blind RBS detector, Cornell geometry

• 1 SDD detector as a relative charge monitor

• 100-200nm Si

3

N

4

window

• Motorized table pos. 10µm

(15)

ERDA-ToF

• ToF and Energy are

measured for each particle in coincidence

• Depth resolution 15 nm

• Mainly used for ERDA on thin films

Mixed Chromium-Silicon oxides

(16)

NRA line

• 25 cm ∅ reaction chamber

• Two gamma-ray detectors (REGe, LaBr3 )

• A detector for backscatterd particles,

• Motorized sample holder (1 axis )

• Tantalum FC, modified HVEE design.

• Control software for authomatic

performance of serial measurements

REGe abs. efficiency

(17)

Quality certification: ISO-9001:2008

Web Information

Annual beamtime planning Beamtime request

Proposal evaluation

Beamtime allocation

Accelerator maintenance Accelerator workplan

Beam delivery User feedback

Registers& Indicators

System main features:

1) Certified 2012-2015, renovated 2015-2018 2) Practically a zero paper system

3) In house development of sofware tools: BT requests, Purchases and providers, Databases

(18)

Training and Dissemination

TRAINING

CMAM PhD students

CMAM Master´s students

International students

Technical school students Support to Master courses

International Training Schemes (IAEA) DISSEMINATION

CMAM Seminars Program Science Week

Guided visists (350 pax per year) Promotional activity UAM Faculty of Science

Scientific Summer Camp

~ 2/year/person

(19)

Support to large facilities

Almost all the activity of the CMAM is focused on analysis and modification of materials.

The nuclear physics line is dedicated both to low energy fundamental research and to test and/or development of experimental set-ups for larger facilities (CERN, FAIR, Ganil, …)

11B(3He,d)ααα

3He(4He,γ)7Be

(20)

Development of a phoswich endcap

19F(p,α)16O*  16Ogs+ γ

Eγ [MeV] Process 6.129 2nd excited 5.618 single escape 5.107 double escape 0.511 annihilation

LaCl3(Ce) LaBr3(Ce) Density [g/cm3] 3.85 5.08 Wavelength of max

emission [nm] 350 380

Refractive index 1.9 1.9

Primary decay time

[ns] 28 16

Light yield

[photons/keV] 49 63

Photoelectron yield

[% of NaI(Tl)] 70-90 165

Resolution @

662keV [%] 3.8 2.9

(21)

Development of a phoswich endcap

The signals from the two detectors are separated by the electronic chain

The energy signal of the slower detector (LaCl3) is gated with region B

(22)

Development of a phoswich endcap

The detector response to high energy pprotons (120-180 MeV, has then be analyzed at the The Svedberg laboratory in Upspala

(23)

Thank you!!!

Referencias

Documento similar