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SCAN META-GGA: THE PREDICTIVE POWER OF 17 EXACT CONSTRAINTS
JOHN P. PERDEW
DEPARMENTS OF PHYSICS AND CHEMISTRY
TEMPLE UNIVERSITY, PHILADELPHIA, PA 19122 USA
ES17, Princeton U., JUNE 27, 2017
SUPPORTED BY NSF-DMR, AND BY DOE-BES THROUGH THE
ENERGY FRONTIER RESEARCH CENTER CCDM.
THE RIGHT ANSWER FOR THE RIGHT REASON AT THE RIGHT PRICE.
NOT AN IMPOSSIBLE DREAM!
HOW CAN WE APPROXIMATE THE DENSITY FUNCTIONAL FOR THE EXCHANGE-CORRELATION ENERGY?
IT IS OFTEN BUT INCORRECTLY SAID THAT βTHERE IS NO SYSTEMATIC WAY TO CONSTRUCT A DENSITY-FUNCTIONAL APPROXIMATIONβ.
THERE IS A SYSTEMATIC OR βPHYSICSβ WAY THAT PRODUCES EXTRAPOLATIVE OR PREDICTIVE FUNCTIONALS.
THERE IS ALSO A βPHYTTINGβ WAY THAT PRODUCES MAINLY INTERPOLATIVE FUNCTIONALS.
FIVE STEPS TO A PHYSICS-BASED DFT APPROXIMATION
(I) PROVE THE EXISTENCE OF THE EXACT DENSITY FUNCTIONAL, AND DERIVE EXACT FORMAL EXPRESSIONS FOR IT.
(II) DISCOVER MATHEMATICAL PROPERTIES OF THE EXACT FUNCTIONAL (EXACT CONSTRAINTS), INCLUDING LIMITS, SCALING RELATIONS, EQUALITIES, AND BOUNDS.
(III) DEVELOP APPROXIMATE BUT COMPUTATIONALLY TRACTABLE FORMS FOR THE APPROXIMATIONS AT VARIOUS LEVELS OF FLEXIBILITY: ADD INGREDIENTS (LSDA, GGA, META-GGA, HYBRID, RPA-LIKE)
(IV) IMPOSE THE EXACT CONSTRAINTS FROM STEP (II) ON A GIVEN FORM, AS APPROPRIATE.
(V) IF A FORM RETAINS SOME FLEXIBILITY, FIT TO APPROPRIATE NORMS, NON-BONDED SYSTEMS FOR WHICH THE FORM CAN BE EXPECTED TO BE ACCURATE.
ALL EXACT CONSTRAINTS ARE CREATED EQUAL, AND ENDOWED BY THEIR CREATOR WITH THE RIGHT TO BE SATISFIED.
STRONGLY CONSTRAINED AND APPROPRIATELY NORMED (SCAN) META-GENERALIZED
GRADIENT APPROXIMATION FOR EXCHANGE AND CORRELATION
CONSTRUCTED VIA STEPS (I)-(V). SATISFIES ALL 17 KNOWN EXACT CONSTRAINTS THAT A META-GGA CAN SATISFY. ITS ACCURACY FOR DIVERSELY-BONDED SYSTEMS CONFIRMS
STEPS (I)-(V).
J. SUN, A. RUZSINSZKY, AND J.P. PERDEW, PRL 2015J. SUN ET AL., NATURE CHEMISTRY 2016
THE 17 EXACT CONSTRAINTS SATISFIED BY SCAN.
AN ASTERISK INDICATES THE 11 EXACT CONSTRAINTS SATISFIED BY PBE.
FOR EXCHANGE:
*1. NEGATIVITY
*2. SPIN SCALING EQUALITY
*3. UNIFORM DENSITY SCALING
4. FOURTH-ORDER GRADIENT EXPANSION
5. FINITE NON-UNIFORM SCALING LIMIT
6. TIGHT LOWER BOUND FOR TWO-ELECTRON DENSITIES
FOR CORRELATION:
*7. NON-POSITIVITY
*8. SECOND-ORDER GRADIENT EXPANSION
*9. UNIFORM DENSITY SCALING TO THE HIGH-DENSITY LIMIT
*10. UNIFORM DENSITY SCALING TO THE LOW-DENSITY LIMIT
11. ZERO CORRELATION ENERGY FOR ONE-ELECTRON DENSITIES
12. FINITE NON-UNIFORM SCALING LIMIT
FOR BOTH:
*13. SIZE EXTENSIVITY
*14. GENERAL LIEB-OXFORD LOWER BOUND
*15. WEAK SPIN-POLARIZATION DEPENDENCE IN LOW-DENSITY LIMIT
*16. STATIC LINEAR RESPONSE OF THE UNIFORM GAS
17. LIEB-OXFORD LOWER BOUND FOR TWO-ELECTRON DENSITIES
INTRODUCTION TO META-GGA
THE ROLE OF π (SPIN SUPPRESSED)
β’ LIMITING FORMS:
β’ SINGLE-ORBITAL SYSTEMS:
ππ€ =1
8|π»π|2/π
β’ UNIFORM ELECTRON GAS (UEG):
ππ’πππ =3
10(3π2)2/3π5/3
REGION πΌ
SINGLE ORBITAL (COVALENT) 0
SLOWLY-VARYING DENSITY (METALLIC)
~1
OVERLAP OF CLOSED SHELLS (NONCOVALENT)
>>1
RIGHT DIMENSIONLESS INGREDIENT FOR MGGA: πΌ =πβππ€
ππ’πππ
),,,,,(],[ 3
nnnnrndnnE xcxcEFFICIENT SEMILOCAL APPROXIMATIONS TO πΈπ₯π:
β’ LSDA: ππ = Οπππππ’π
|ππ,π|2
β’ GGA: ADDS π»πβ AND π»πββ’ MGGA: ADDS ππ = Οπ
ππππ’π 1
2|π»ππ,π|
2
β’ ππ,π βΆ KOHN β SHAM ORBITALS
G3 (kcal/mol) BH76 (kcal/mol)
S22 (kcal/mol) LC20 (β«)
ME MAE ME MAE ME MAE ME MAE
GGA
PBE 22.2 9.2 2.8 0.059
MGGA SCAN - 5.7 7.7 - 0.9 0.016
-
EARLY RESULTS FOR MOLECULES AND SOLIDS
MAE: MEAN ABSOLUTE ERROR
G3: ATOMIZATION ENERGIES OF 223 MOLECULES
BH76: 76 REACTION BARRIERS
S22: 22 MOLECULAR COMPLEXES BOUND BY WEAK BONDS
LC20: LATTICE CONSTANTS OF 20 SOLIDS INCLUDING METALS, SEMICONDUCTORS, AND INSULATORS
THE NONEMPIRICAL SCAN META-GGA IS MORE ACCURATE THAN THE NONEMPIRICAL PBE GGA, ESPECIALLY FOR WEAK BONDS AND INTERMEDIATE-RANGE VAN DER WAALS ATTRACTION. (SOFT MATTER AS WELL AS HARD!)
NOTE THAT SCAN IS NOT FITTED TO ANY BONDED SYSTEM. THUS ITS RESULTS FOR BONDS ARE GENUINE PREDICTIONS, NOT FITS.
Phase transition pressure and defect formation energies of Si: The situation before SCAN
STRUCTURAL PHASE TRANSITIONINTERSTITIAL DEFECT FORMATION ENERGY
REF: E.R. Batista, et al, PRB, 74, 121102 (2006)
PERFORMANCE OF SCAN FOR SOLID Si
Phase transition Interstitial defect formation (eV)
πΏπΈ(meV) ππ‘(Gpa) X H T
PBE 290 8.4 3.61 3.65 3.78
SCAN 411 14.3 4.29 4.36 4.59
Ref 480Β±50 11-15 4.5-4.8
ENERGETIC ORDERING OF WATER HEXAMERS(BINDING ENERGY IN meV/H2O)
method Prism Cage Book Cyclic
DMC 331.9 329.5 327.8 320.8
CCSD(T) 347.6 345.5 338.9 332.5
PBE 336.1 339.4 345.6 344.1
SCAN 376.8 375.6 370.0 359.7
PBE+vd
W(TS) 369.6 372.6 370.6 360.7
Ref: B. Santra, et al, JCP, 129, 194111 (2008)
~7 ICE PHASES: CORRECT ENERGY DIFFERENCES
LIQUID WATER BY AB INITIO MOLECULAR DYNAMICS:
PBE OVERSTRUCTURES WATER, AND MAKES ICE SINK IN WATER. SCAN CORRECTS THESE ERRORS. WATER IS ESSENTIAL FOR CHEMISTRY AND BIOLOGY.
TESTED FERROELECTRICS/MULTIFERROICS: SCAN MUCH BETTER THAN PBE FOR STRUCTURAL DISTORTIONS, POLARIZATIONS, AND TRANSITION TEMPERATURES.
STABILITIES OF CRYSTAL STRUCTURES
WORK WITH GERD CEDER SHOWS THAT SCAN HALVES THE ERRORS OF PBE FOR FORMATION ENERGIES OF 200 BINARY SOLIDS AND FOR PREDICTION OF THE GROUND-STATE CRYSTAL STRUCTURES.
SCAN BAND GAPS OF SOLIDS IN A GKS SCHEME ARE LESS UNDERESTIMATED THAN PBE GAPS, AND (FOR STRONGLY-CORRELATED SYSTEMS) OFTEN CLOSE TO PBE+U GAPS.
BUT HYBRID GAPS IN GKS ARE EVEN BETTER. ALL FOR THE RIGHT REASON. (PERDEW, YANG, BURKE ET AL., PNAS, 2017)
NONLOCAL CORRECTIONS TO SCAN
(1) LONG-RANGE VAN DER WAALS INTERACTION(SCAN+rVV10). IMPORTANT FOR THE EXFOLIATION ENERGIES OFLAYERED MATERIALS,
AND FOR THE SURFACE ENERGIES AND WORK FUNCTIONS OF METALS.
H. PENG, Z. YANG, J. SUN, & J.P. PERDEW, PHYS. REV. X (2016)
(2) SELF-INTERACTION CORRECTION, PIECEWISE LINEARITY OF E(N), FLAT PLANE CONDITION (UNDER DEVELOPMENT).
NEEDED FOR STRETCHED BONDS OR STRONG CORRELATION.
SUMMARY OF SCAN
β’ A META-GGA, STRONGLY CONSTRAINED AND APPROPRIATELY NORMED.
β’ COMPUTATIONALLY EFFICIENT AND NONEMPIRICAL. AVAILABLE IN VASP, ADF, QCHEM, QUANTUM ESPRESSO,β¦
β’ SYSTEMATIC IMPROVEMENT OVER THE PBE GGA FOR A WIDE RANGE OF PROPERTIES.
β’ OFTEN PERFORMS LIKE A HYBRID FUNCTIONAL, AT LOWER COST AND WITH INTERMEDIATE-RANGE VAN DER WAALS INTERACTION.
LONG-RANGE vdW INTERACTION FROM SCAN+rVV10. SELF-INTERACTION CORRECTIONS TO SCAN (SATISFYING THE LAST KNOWN EXACT CONSTRAINTS) ARE UNDER DEVELOPMENT.
EXCHANGE
EXACT CONSTRAINTS
πΈπ₯ππΆπ΄π π = ΰΆ±π3ππππ₯
π’πππ(π)πΉπ₯
ππΆπ΄π(π , πΌ)
πΉπ₯ππΆπ΄π π , πΌ = {βπ₯
1 π , πΌ + ππ₯ πΌ [βπ₯0 β βπ₯
1 π , πΌ ]}ππ₯ π
UNDETERMINED PARAMETERS: π1, π1x, π2x, πx
1. TIGHT LOWER BOUND FOR EXCHANGE πΉπ₯ππΆπ΄π β€ 1.174 β βπ₯
0=1.174
3. NON-UNIFORM SCALING LIMIT: limπ ββ
πΉπ₯ππΆπ΄π π , πΌ β π β
1
2 β ππ₯ π = 1 β πΈπ₯π[βπ1π β1/2]
2. 4TH-ORDER GRADIENT EXPANSION OF SLOWLY VARYING DENSITY LIMIT (π β0 and πΌ β1):
πΉπ₯GE4 π , πΌ = 1 +
10
81π 2 β
1606
18225π 4 +
511
13500π 2 1 β πΌ +
5913
405000(1 β πΌ)2
RESUMMATION OF 4TH-ORDER GRADIENT EXPANSION (RGE):
βπ₯1 π , πΌ = 1 + π1 β
π1
1 +ππ΄πΎπ
2(1 +π4 π 2/ππ΄πΎπΈπ₯π(β|π4|π
2/ππ΄πΎ)) + {π1π 2 + π2 1 β πΌ πΈπ₯π βπ3 1 β πΌ
2 }2
π1
π1=4.9479: Ex(H)
INTERPOLATION AND EXTRAPOLATION: ππ₯ πΌ = πΈπ₯π βπ1xπΌ
1βπΌπ 1 β πΌ β πxπΈπ₯π
π2x
1βπΌπ πΌ β 1
ππ΄πΎ = 10/81, π1 =0.156632, π2 = 0.12083, π3 = 0.5, π4 =ππ΄πΎ2
π1β 0.112654
NO CORRECTION TO RGE IN ANY POWER OF π»π AT THE SLOWLY VARYING DENSITY LIMIT
π(π₯): STEP FUNCTION
3/12 )3)(4/3()( nnunifx 3/43/12 )()3(2
||
n
ns
CORRELATION
EXACT CONSTRAINTS
UNDETERMINED PARAMETERS: π1c, π2c, ππ
1. ONE ELECTRON SELF-CORRELATION FREE
3. 2ND-ORDER GRADIENT EXPANSION OF SLOWLY VARYING DENSITY LIMIT β A SIMPLIFIED PBE CORRELATION FOR ππ1
INTERPOLATION AND EXTRAPOLATION: ππ πΌ = πΈπ₯π βπ1cπΌ
1βπΌπ 1 β πΌ β πcπΈπ₯π
π2c
1βπΌπ πΌ β 1
πΈπππΆπ΄π π = ΰΆ±π3ππππ
ππΆπ΄π )ππππΆπ΄π = ππ
1 + ππ πΌ (ππ0 β ππ
1
2. LOWER BOUND ON πΈπ₯π OF 2-ELECTRON DENSITIES: πΈπ₯π π β₯ 1.67πΈπ₯πΏπ·π΄
NONEMPIRICAL ππ0
4. NON-POSITIVITY β ππ0 β₯ ππ
1