Characterisation Ch t i ti of f mesopores ortho-Positronium m lifetime f m measurement on controlled pore glass S Thraenert1, D. S. D Enke2, R. Krause-Rehberg1 Martin-Luther-Universität Halle-Wittenberg g Naturwissenschaftliche Fakultät II 1Institut für Physik 2Institut für Chemie Outline Porous glass - CPG Principles of PALS 0.018 0.016 0.012 1000000 the model calibration curve pore size distribution p Summary 1.8 nm 0.014 100000 E Experimental i t l results lt 0.020 From τ4 to pore size d positron and d positronium lifetime measurement the spectrum pdf n(d) synthesis y properties 2.5 nm 0.010 4.5 nm 0.008 0.006 6 2 nm 6.2 0.004 10000 0.002 N 0.000 0 1000 5 10 8 nm 15 d(nm) 100 40 nm 10 0 100 200 300 400 500 600 700 800 900 t (ns) o-Ps lifetime measurement on CPG 2 Controlled pore glass - CPG VYCOR-Process alkali borosilicate glass l Extraction T 530 – 710°C HCl/NaOH dP 1 to 110 nm spinodal phase separation decomposition is initiated by heat treatment alkali rich borate phase <-> pure silica alkali phase soluble in acid -> silica network pore size depends on basic material porosity of 50 % F. Janowski, D. Enke in F. Schüth, K.S.W. Sing, J. Weitkamp (Eds.), Handbook of Porous Solids, WILEY-VCH, Weinheim, 2002, 1432-1542. o-Ps lifetime measurement on CPG 3 Controlled pore glass - CPG different geometries p possible homogenous microstructure uniform pore size controlled pore size we can choose d (!) D. Enke, F. Janowski, W. Schwieger, Microporous and Mesoporous Materials 2003, 60, 19-30. o-Ps lifetime measurement on CPG 4 Outline Porous glass - CPG Principles of PALS 0.018 0.016 0.012 1000000 the model calibration curve pore size distribution p Summary 1.8 nm 0.014 100000 E Experimental i t l results lt 0.020 From τ4 to pore size d positron and d positronium lifetime measurement the spectrum pdf n(d) synthesis y properties 2.5 nm 0.010 4.5 nm 0.008 0.006 6 2 nm 6.2 0.004 10000 0.002 N 0.000 0 1000 5 10 8 nm 15 d(nm) 100 40 nm 10 0 100 200 300 400 500 600 700 800 900 t (ns) o-Ps lifetime measurement on CPG 5 Principles of PALS: PALS pick-off annihilation positrons from 22Na: thermalize, diffuse, being pp and annihilate trapped OR: positrons form Ps 25 % pick-off annihilation: o-Ps captures e- with anti-parallel spin h happens during d i collisions lli i att walls ll of f pore lifetime (τ) decreases rapidly τ is function of p pore size: 1.5 - 142 ns also for closed pore systems 75 % positronium: p-Ps -> short self annihilation lifetime of 0.125 ns o-Ps -> long self annihilation lifetime of 142 ns (3γ) ->> pick off annihilation (2γ) o-Ps lifetime measurement on CPG 6 Principles of PALS sample preparation: ”sandwich” positron(ium) lifetime: time between “birth” birth” (1,27 (1 27 MeV) and “death” death” (511 keV) 10 6 10 5 10 4 10 3 10 2 10 1 5 nm 26 nm 0 200 400 600 800 time (ns) o-Ps lifetime measurement on CPG 7 Principles of PALS: typical spectrum typical lifetime spectrum for CPG (here d = 20 nm): 4 exponential ti l d decay components t p-Ps -> 0.125 ns free positrons ~ 0.5 ns o-Ps in disordered structure ~ 1.5 ns o-Ps in pores analysis with LT9 (LifeTime) o-Ps lifetime measurement on CPG 8 Outline Porous glass - CPG Principles of PALS 0.018 0.016 0.012 1000000 the model calibration curve pore size distribution p Summary 1.8 nm 0.014 100000 E Experimental i t l results lt 0.020 From τ4 to pore size d positron and d Positronium lifetime measurement the spectrum pdf n(d) synthesis y properties 2.5 nm 0.010 4.5 nm 0.008 0.006 6 2 nm 6.2 0.004 10000 0.002 N 0.000 0 1000 5 10 8 nm 15 d(nm) 100 40 nm 10 0 100 200 300 400 500 600 700 800 900 t (ns) o-Ps lifetime measurement on CPG 9 Extended Tao Eldrup model extended TE model (calculations by EELViS): quantum well of infinite height, but: overlap of o-Ps wave function and wall of pore -> δ Boltzmann statistics ascribes explicit p temperature p dependence p to the lifetime integrals of spherical / cylindrical Bessel functions δ = 0.19 nm mean free path D = 4V/S = dcyl, diameter of cylinder mean free f path th D = 4V/S = 2/3 dsphere, diameter di t of f sphere h R. Zaleski, Excited Energy Levels and Various Shapes (EELViS), Institute of Physics, Maria Curie-Sklodowska University, Lublin, Poland o-Ps lifetime measurement on CPG 10 Outline Porous glass - CPG Principles of PALS 0.018 0.016 0.012 1000000 the model calibration curve pore size distribution p Summary 1.8 nm 0.014 100000 E Experimental i t l results lt 0.020 From τ4 to pore size d positron and d Positronium lifetime measurement the spectrum pdf n(d) synthesis y properties 2.5 nm 0.010 4.5 nm 0.008 0.006 6 2 nm 6.2 0.004 10000 0.002 N 0.000 0 1000 5 10 8 nm 15 d(nm) 100 40 nm 10 0 100 200 300 400 500 600 700 800 900 t (ns) o-Ps lifetime measurement on CPG 11 The experiments at T = 300 K o-Ps lifetime measurement on CPG we measured CPG in a broad pore size range given pore sizes obtained by N2-adsorption adsorption or Hg Hg-intrusion intrusion δ = 0.193 nm best fit for our CPG -> calibration curve for calculating pore size g good model for T = 300 K, also good model for temperature dependence of lifetime? 12 The T-dependence calculations: cylindric model with δ = 0.193 nm although we found good agreement for T > 300 K temperature behavior cannot be explained very well at low temperatures for 20 nm a catching effect of o-Ps at low temperatures may occur (van-der-waals power, “capillary “ ill condensation”) and o-Ps bonds at the wall model still too simple but works well for room temperature o-Ps lifetime measurement on CPG 13 τ4 (ns) Pore size distribution 140 D 120 1.8 nm 100 τ4 80 ETE models spheres with δ = 0.19 nm cappillars ill with ith δ = 0.193 0 193 nm experiment σ4 (ns)) 60 40 σ4 20 0 1 10 100 pore size D = 4V/S (nm) from porosimetry o-Ps lifetime measurement on CPG τ4 σ4 21.1 ns 14.8 ns 2.5 nm 46.9 ns 17.6 ns 4 5 nm 4.5 65 9 ns 65.9 18 9 ns 18.9 6.2 nm 80.0 ns 19.3 ns τ4 and its distribution σ4 by analysis of truncated spectra starting from 20 ns problem of LT: limit of 142 ns is not taken into account, for large pores unphysically large σ4 distribution for 4 smaller selected pores 14 Pore size distribution , α4(λ) is probability density function (pdf) of o-Ps annihilation rate, assumed by LT to be a log. Gaussian from distr. α4(τ) it is possible to calc. distribution of diameters of the pore: ⎛ dτ 4 n(d cyl ) = α 4 (τ )⎜ ⎜ dd ⎝ cyl 0.012 0.010 0.006 4.5 nm 0 004 0.004 6.2 nm 0.002 0.000 0 20 40 60 80 100 120 τ(ns) ⎞ ⎟ ⎟ ⎠ all we need is a differentiable analytical function τ4 = τ4(dcyl): 2.5 nm 0.008 140 120 100 τ4 (ns) 1.8 nm 0.014 2 distribution of τ4: α4(τ) = α4(λ)λ2 pd df α4(τ) = α4(λ)λ 0.016 ⎛ ⎞ A1 − A2 ⎜ ⎟ τ 4 = A2 + ⎜ p ⎟ ⎝ 1 + (d cyl / d cyl 0 ) ⎠ ETE Fit 80 60 40 20 0 1 10 100 d (nm) o-Ps lifetime measurement on CPG 15 Pore size distribution 0.020 0.018 0.016 1.8 nm 0.014 pdf n(d) 0.012 2.5 nm 0.010 4.5 nm 0.008 0.006 6 2 nm 6.2 0.004 0.002 0.000 5 0 ,1 2 VPore (cm3g-1) 0 ,1 0 0 ,0 8 0 ,0 6 d ((n m ) 10 pore size distribution from BJH method (N2 ads.) for the same 4.5 nm sample volume weighted 15 0 ,0 6 0 ,0 4 0 ,0 4 0 ,0 2 dV/dr (cm3nm-1g-1) 0 0 ,0 2 0 ,0 0 0 5 10 distribution norm. to 1 arrows show d directly calculated from mean o-Ps lifetime using cylindric model (1.77 nm, 3.09 nm, 4.38 nm and 5.80 nm) this distribution contains the true variation of pore sizes but also the effect of irregular not linear character of pores long tail for larger pores: overestimation of f α4((τ)) nonlinear char. τ4 vs. d 0 ,0 0 15 d ((n m ) to be published o-Ps lifetime measurement on CPG 16 Outline Porous glass - CPG Principles of PALS 0.018 0.016 0.012 1000000 the model calibration curve pore size distribution p Summary 1.8 nm 0.014 100000 E Experimental i t l results lt 0.020 From τ4 to pore size d positron and d Positronium lifetime measurement the spectrum pdf n(d) synthesis y properties 2.5 nm 0.010 4.5 nm 0.008 0.006 6 2 nm 6.2 0.004 10000 0.002 N 0.000 0 1000 5 10 8 nm 15 d(nm) 100 40 nm 10 0 100 200 300 400 500 600 700 800 900 t (ns) o-Ps lifetime measurement on CPG 17 Summary for T = 300 K we found a calibration curve for CPG non destructive porosimetry tool for opened and closed pore-systems most sensitive for d = 0.5 … 10 nm for other temperatures the measurements show disagreement to the ETE model -> model still too simple for pores d < 10 nm we can calculate a pore size distribution near future: f t phase transition of gas in CPG (to be presented @ PPC9 Wuhan / China, May 2008) SBA-15 (to be presented @ COPS VIII Edinburgh / Scotland, June 2008) 0.020 0.018 0.016 1.8 nm 0.014 0.012 pdf n(d) 2.5 nm 0.010 4.5 nm 0.008 0.006 6.2 nm 0.004 0.002 0.000 0 5 10 15 d(nm) o-Ps lifetime measurement on CPG 18 Acknowledgment Special thanks from our group go to: R. Zaleski and his group R (Lublin/Poland) for EELViS G. Dlubek (Halle/Germany) for fruitful discussions all organizers of DZT20 o-Ps lifetime measurement on CPG 19 Thanks for your patience! This talk as pdf? http://positron physik uni halle de http://positron.physik.uni-halle.de o-Ps lifetime measurement on CPG 20