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Loss mechanisms
in Polymer-Fullerene Solar Cells
Carsten Deibel
Julius-Maximilians-University of Würzburg
223rd ECS meeting, Toronto
15th May 2013
deibel@disorderedmatter.eu
How Do Organic Solar Cells Work?
2
Step 1: Light Absorption
➟ Exciton Generation in Polymer
Fullerene
Aluminium Cathode
Transparent Anode
Polymer
Voltage
Current
How Do Organic Solar Cells Work?
3
Step 2: Exciton Diffusion
➟ to Acceptor Interface
Fullerene
Aluminium Cathode
Transparent Anode
Polymer
Voltage
Current
singlet losses
Step 3: Exciton Dissociation
➟ Polaron Pair Generation
How Do Organic Solar Cells Work?
4
Fullerene
Aluminium Cathode
Transparent Anode
Polymer
charge transfer:
very fast and
very efficient
Voltage
Current
singlet losses
How Do Organic Solar Cells Work?
5
Step 4: Polaron Pair Dissociation
➟ Free Electron–Hole Pairs!
Fullerene
Aluminium Cathode
Transparent Anode
Polymer
Voltage
Current
singlet losses
geminate losses
How Do Organic Solar Cells Work?
6
Step 5: Charge Transport
➟ Photocurrent
Fullerene
Aluminium Cathode
Transparent Anode
Polymer
Voltage
Current
singlet losses
geminate losses
nongeminate losses
for instance, PTB7:PC70BM 1:1.5
What are we looking at?
7
glass
PEDOT
V












additive DIO
for instance, PTB7:PC70BM 1:1.5
What are we looking at?
7
300
200
100
0
-100
currentdensity[A/m
2
]
0.80.60.40.20.0
voltage [V]
dark 1 sun
w/o add
with add
PCE [%] FF [%]
w/o add 3.8 51
with add 7.1 69
glass
PEDOT
V
PTB7:PC70BM 1:1.5 Morphology
8
phase
height
w/o additive, 3.8%
Alex Förtig
nm
nm
with additive, 7.1%
PTB7:PC70BM 1:1.5 Morphology
8
phase
height
w/o additive, 3.8%
Alex Förtig
nm
nm
Which processes are
limiting the
performance of these
organic solar cells?
Outline
10
Outline
10
conclusions
implications on organic
solar cell performance
nongeminate
recombination
with additive
geminate
recombination
without additive
Outline
10
conclusions
implications on organic
solar cell performance
nongeminate
recombination
with additive
geminate
recombination
without additive
j(V ) = e
Z
(G R) dx
⇡ jgen jloss(V )
jgen ⇡ jsc
Current–Voltage Reconstruction ...
11
From the continuity equation:
Voltage
Current
jloss(V ) /
n(V )
⌧(n)
12
n(V) by charge extraction
act of Solvent Additive on PTB7:PC71BM Solar Cells 65
2
4
10
21
2
4
10
22
0.80.60.40.20.0
voltage [V]
10
21
2
4
10
22
2
4
chargecarrierdensity[m
-3
]
with add
w/o add
0.03 sun
1 sun
: Voltage dependent charge carrier density n(V ) from charge ex-
periments for PTB7:PC71BM devices with and without additive at
Alex Förtig
jloss(V ) /
n(V )
⌧(n)
Nongem. Loss Current
τ(n) by transient photovoltage
12
n(V) by charge extraction
act of Solvent Additive on PTB7:PC71BM Solar Cells 65
2
4
10
21
2
4
10
22
0.80.60.40.20.0
voltage [V]
10
21
2
4
10
22
2
4
chargecarrierdensity[m
-3
]
with add
w/o add
0.03 sun
1 sun
: Voltage dependent charge carrier density n(V ) from charge ex-
periments for PTB7:PC71BM devices with and without additive at
with add.
4
6
8
10
2
4
6
8
100
lifetime[µs]
3 4 5 6 7 8 9
10
22
2
charge carrier density [m
-3
]
1sun
1sun
w/out add.
Alex Förtig
jloss(V ) /
n(V )
⌧(n)
Nongem. Loss Current
reconstruction works well
... with Additive
Origin of nongeminate
recombination?
13
-150
-100
-50
0
50
CurrentDensity[A/m
2
]
0.60.40.20.0
Voltage [V]
meas. PL reconstr.
1 sun
0.32 sun
0.03 sun
Alex Förtig
LUMO
HOMO
(1)
(2)
(1)
expected in nongeminate loss in low mobility materials
Langevin Recombination
(1) finding of charge carriers → mobility μ
(2) recombination event (faster than (1))
14
R(n) / µ(n)n2
}
Expected:
Back to PTB7: Expected vs Observed
15Adv. Funct. Mater. 2, 1483 (2012)
3
4
5
6
7
8
9
10
-20
2
3
µ[Am]
4 6 8
10
21
2 4 6 8
10
22
2 4 6 8
10
23
charge carrier density [m
-3
]
10
-18
2
3
4
5
6
7
8
9
10
-17
k[m
3
s
-1
]
PTB7:PC!
with additive
71BM
~
T=300 K
Expected:
Back to PTB7: Expected vs Observed
15Adv. Funct. Mater. 2, 1483 (2012)
3
4
5
6
7
8
9
10
-20
2
3
µ[Am]
4 6 8
10
21
2 4 6 8
10
22
2 4 6 8
10
23
charge carrier density [m
-3
]
10
-18
2
3
4
5
6
7
8
9
10
-17
k[m
3
s
-1
]
PTB7:PC!
with additive
71BM
~
T=300 K
Expected:
Back to PTB7: Expected vs Observed
15Adv. Funct. Mater. 2, 1483 (2012)
3
4
5
6
7
8
9
10
-20
2
3
µ[Am]
4 6 8
10
21
2 4 6 8
10
22
2 4 6 8
10
23
charge carrier density [m
-3
]
10
-18
2
3
4
5
6
7
8
9
10
-17
k[m
3
s
-1
]
PTB7:PC!
with additive
71BM
~
T=300 K
6/
Expected:
Back to PTB7: Expected vs Observed
15Adv. Funct. Mater. 2, 1483 (2012)
3
4
5
6
7
8
9
10
-20
2
3
µ[Am]
4 6 8
10
21
2 4 6 8
10
22
2 4 6 8
10
23
charge carrier density [m
-3
]
10
-18
2
3
4
5
6
7
8
9
10
-17
k[m
3
s
-1
]
PTB7:PC!
with additive
71BM
~
T=300 K
Trap Tail States by Thermally Stimulated Currents
Trapping is Important
Trap density = Lower Limit
Shape roughly exponential,
energy tail ~90 meV
16Julia Rauh
10
21
2
3
4
5
6
7
8
9
10
22
trapdensity[m
-3
]
0.300.250.200.150.100.050.00
Energy [eV]
PTB7:PC70BM
with DIO
Transient Absorption
Nongeminate Decay Dynamics
17
4
6
8
10
-5
2
4
6
8
10
-4
2
4
6
8
ΔOD[a.U]
10
-7
10
-6
10
-5
10
-4
10
-3
Time [s]
PTB7:PC71BM
with additive
300K 150K
4.5K
Clemens Grünewald, Julia Kern
Transient Absorption
Nongeminate Decay Dynamics
17
4
6
8
10
-5
2
4
6
8
10
-4
2
4
6
8
ΔOD[a.U]
10
-7
10
-6
10
-5
10
-4
10
-3
Time [s]
PTB7:PC71BM
with additive
300K 150K
4.5K
fast free–free
(Langevin type)
recombination
Clemens Grünewald, Julia Kern
Transient Absorption
Nongeminate Decay Dynamics
17
4
6
8
10
-5
2
4
6
8
10
-4
2
4
6
8
ΔOD[a.U]
10
-7
10
-6
10
-5
10
-4
10
-3
Time [s]
PTB7:PC71BM
with additive
300K 150K
4.5K
fast free–free
(Langevin type)
recombination
slow free–trapped
recombination
Clemens Grünewald, Julia Kern
Outline
18
conclusions
implications on organic
solar cell performance
nongeminate
recombination
with additive
geminate
recombination
without additive
PTB7:PC70BM 1:1.5 w/o additive
I–V Reconstruction
Why?
19
reconstruction incomplete
j(V ) = jsc jloss (n(V ))
-50
-40
-30
-20
-10
0
10
CurrentDensity[A/m
2
]
0.80.60.40.2
Voltage [V]
meas. PL reconstr.
0.56 sun
0.32 sun
0.18 sun
0.03 sun
PTB7:PC70BM 1:1.5 w/o additive
I–V Reconstruction
Why?
19
reconstruction incomplete
j(V ) = jsc jloss (n(V ))
-50
-40
-30
-20
-10
0
10
CurrentDensity[A/m
2
]
0.80.60.40.2
Voltage [V]
meas. PL reconstr.
0.56 sun
0.32 sun
0.18 sun
0.03 sun
1.0
0.8
0.6
0.4
0.2
measured/reconstructed
0.80.60.40.2
Voltage [V]
ratio PL Voc
0.03 sun
0.18 sun
0.32 sun
0.56 sun
1 sun
First try:
Time Delayed Collection Field → P(V)
Main Reason: Photogeneration
w/out additive: voltage
dependent photogeneration
20Alex Förtig
5
6
7
8
9
1
Qtot/Q(-5V)
-5 -4 -3 -2 -1 0
prebias voltage [V]
w/o add
data
fit
with add
data origin unclear
j(V ) = e
Z
(G R) dx
⇡ jgen jloss(V )
jgen ⇡ jsc
Current–Voltage Reconstruction ...
21
From the continuity equation:
Voltage
Current
jloss(V ) /
n(V )
⌧(n)
j(V ) = e
Z
(G R) dx
⇡ jgen(V ) jloss(V )
Current–Voltage Reconstruction ...
22
From the continuity equation:
jloss(V ) /
n(V )
⌧(n)
Voltage
Current
jgen(V ) ⇡ jsc · P(V )
Time Delayed Collection Field
Reconstruction incl. Geminate Loss
23
5
6
7
8
9
1
Qtot/Q(-5V)
-5 -4 -3 -2 -1 0
prebias voltage [V]
w/o add
data
fit
with add
data
Time Delayed Collection Field
Reconstruction incl. Geminate Loss
23
5
6
7
8
9
1
Qtot/Q(-5V)
-5 -4 -3 -2 -1 0
prebias voltage [V]
w/o add
data
fit
with add
data
-80
-60
-40
-20
0
currentdensity[A/m
2
]
0.80.60.40.2
voltage [V]
0.18 sun
1 sun
w/o Add
measurement
reconstruction
j (V)gen
2
4
10
21
2
4
10
22
0.80.60.40.20.0
voltage [V]
10
21
2
4
10
22
2
4
chargecarrierdensity[m
-3
]
with add
w/o add
0.03 sun
1 sun
What if...
reverse reconstruction:

 n(V) from I(V)
24Alex Förtig
incomplete extraction
„Nanomorphology“ by PL
25Björn Gieseking
1.0
0.8
0.6
0.4
0.2
0.0
Photoluminescence(norm.)
2.01.81.61.41.2
Energy / eV
1.0
0.5
0.0
1100 1000 900 800 750 700 650
Wavelength / nm
w/o add.3 % DIO
PTB7 PC71BM
„Nanomorphology“ by PL
additive: relative decrease of
fullerene PL
→ smaller fullerene domains
25Björn Gieseking
1.0
0.8
0.6
0.4
0.2
0.0
Photoluminescence(norm.)
2.01.81.61.41.2
Energy / eV
1.0
0.5
0.0
1100 1000 900 800 750 700 650
Wavelength / nm
w/o add.3 % DIO
PTB7 PC71BM
...on fullerene islands
Scenario: Spatial Trapping...
without additive
26
Fullerene
Polymer
Aluminium Cathode
Transparent Anode
Fullerene
Polymer
Aluminium Cathode
Transparent Anode
with additive
Conclusions
27
with additive, 7.1% w/o additive, 3.8%












Conclusions
27
with additive, 7.1% w/o additive, 3.8%












nongeminate recombination
free carrier and trap assisted
recombination
Conclusions
27
with additive, 7.1% w/o additive, 3.8%












nongeminate recombination
free carrier and trap assisted
recombination
geminate & nongeminate
field dependent
photogeneration
spatial trapping
on fullerene
Thanks to Prof.
Dyakonov and
Würzburg group!
Thank you!
deibel@disorderedmatter.eu
Bayerische
Akademie der Wissenschaften
EU, DBU, Elite network Bavaria

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Loss mechanisms in Polymer-Fullerene Solar Cells

  • 1. Loss mechanisms in Polymer-Fullerene Solar Cells Carsten Deibel Julius-Maximilians-University of Würzburg 223rd ECS meeting, Toronto 15th May 2013 deibel@disorderedmatter.eu
  • 2. How Do Organic Solar Cells Work? 2 Step 1: Light Absorption ➟ Exciton Generation in Polymer Fullerene Aluminium Cathode Transparent Anode Polymer Voltage Current
  • 3. How Do Organic Solar Cells Work? 3 Step 2: Exciton Diffusion ➟ to Acceptor Interface Fullerene Aluminium Cathode Transparent Anode Polymer Voltage Current singlet losses
  • 4. Step 3: Exciton Dissociation ➟ Polaron Pair Generation How Do Organic Solar Cells Work? 4 Fullerene Aluminium Cathode Transparent Anode Polymer charge transfer: very fast and very efficient Voltage Current singlet losses
  • 5. How Do Organic Solar Cells Work? 5 Step 4: Polaron Pair Dissociation ➟ Free Electron–Hole Pairs! Fullerene Aluminium Cathode Transparent Anode Polymer Voltage Current singlet losses geminate losses
  • 6. How Do Organic Solar Cells Work? 6 Step 5: Charge Transport ➟ Photocurrent Fullerene Aluminium Cathode Transparent Anode Polymer Voltage Current singlet losses geminate losses nongeminate losses
  • 7. for instance, PTB7:PC70BM 1:1.5 What are we looking at? 7 glass PEDOT V             additive DIO
  • 8. for instance, PTB7:PC70BM 1:1.5 What are we looking at? 7 300 200 100 0 -100 currentdensity[A/m 2 ] 0.80.60.40.20.0 voltage [V] dark 1 sun w/o add with add PCE [%] FF [%] w/o add 3.8 51 with add 7.1 69 glass PEDOT V
  • 9. PTB7:PC70BM 1:1.5 Morphology 8 phase height w/o additive, 3.8% Alex Förtig nm nm
  • 10. with additive, 7.1% PTB7:PC70BM 1:1.5 Morphology 8 phase height w/o additive, 3.8% Alex Förtig nm nm
  • 11. Which processes are limiting the performance of these organic solar cells?
  • 13. Outline 10 conclusions implications on organic solar cell performance nongeminate recombination with additive geminate recombination without additive
  • 14. Outline 10 conclusions implications on organic solar cell performance nongeminate recombination with additive geminate recombination without additive
  • 15. j(V ) = e Z (G R) dx ⇡ jgen jloss(V ) jgen ⇡ jsc Current–Voltage Reconstruction ... 11 From the continuity equation: Voltage Current jloss(V ) / n(V ) ⌧(n)
  • 16. 12 n(V) by charge extraction act of Solvent Additive on PTB7:PC71BM Solar Cells 65 2 4 10 21 2 4 10 22 0.80.60.40.20.0 voltage [V] 10 21 2 4 10 22 2 4 chargecarrierdensity[m -3 ] with add w/o add 0.03 sun 1 sun : Voltage dependent charge carrier density n(V ) from charge ex- periments for PTB7:PC71BM devices with and without additive at Alex Förtig jloss(V ) / n(V ) ⌧(n) Nongem. Loss Current
  • 17. τ(n) by transient photovoltage 12 n(V) by charge extraction act of Solvent Additive on PTB7:PC71BM Solar Cells 65 2 4 10 21 2 4 10 22 0.80.60.40.20.0 voltage [V] 10 21 2 4 10 22 2 4 chargecarrierdensity[m -3 ] with add w/o add 0.03 sun 1 sun : Voltage dependent charge carrier density n(V ) from charge ex- periments for PTB7:PC71BM devices with and without additive at with add. 4 6 8 10 2 4 6 8 100 lifetime[µs] 3 4 5 6 7 8 9 10 22 2 charge carrier density [m -3 ] 1sun 1sun w/out add. Alex Förtig jloss(V ) / n(V ) ⌧(n) Nongem. Loss Current
  • 18. reconstruction works well ... with Additive Origin of nongeminate recombination? 13 -150 -100 -50 0 50 CurrentDensity[A/m 2 ] 0.60.40.20.0 Voltage [V] meas. PL reconstr. 1 sun 0.32 sun 0.03 sun Alex Förtig
  • 19. LUMO HOMO (1) (2) (1) expected in nongeminate loss in low mobility materials Langevin Recombination (1) finding of charge carriers → mobility μ (2) recombination event (faster than (1)) 14 R(n) / µ(n)n2 }
  • 20. Expected: Back to PTB7: Expected vs Observed 15Adv. Funct. Mater. 2, 1483 (2012) 3 4 5 6 7 8 9 10 -20 2 3 µ[Am] 4 6 8 10 21 2 4 6 8 10 22 2 4 6 8 10 23 charge carrier density [m -3 ] 10 -18 2 3 4 5 6 7 8 9 10 -17 k[m 3 s -1 ] PTB7:PC! with additive 71BM ~ T=300 K
  • 21. Expected: Back to PTB7: Expected vs Observed 15Adv. Funct. Mater. 2, 1483 (2012) 3 4 5 6 7 8 9 10 -20 2 3 µ[Am] 4 6 8 10 21 2 4 6 8 10 22 2 4 6 8 10 23 charge carrier density [m -3 ] 10 -18 2 3 4 5 6 7 8 9 10 -17 k[m 3 s -1 ] PTB7:PC! with additive 71BM ~ T=300 K
  • 22. Expected: Back to PTB7: Expected vs Observed 15Adv. Funct. Mater. 2, 1483 (2012) 3 4 5 6 7 8 9 10 -20 2 3 µ[Am] 4 6 8 10 21 2 4 6 8 10 22 2 4 6 8 10 23 charge carrier density [m -3 ] 10 -18 2 3 4 5 6 7 8 9 10 -17 k[m 3 s -1 ] PTB7:PC! with additive 71BM ~ T=300 K
  • 23. 6/ Expected: Back to PTB7: Expected vs Observed 15Adv. Funct. Mater. 2, 1483 (2012) 3 4 5 6 7 8 9 10 -20 2 3 µ[Am] 4 6 8 10 21 2 4 6 8 10 22 2 4 6 8 10 23 charge carrier density [m -3 ] 10 -18 2 3 4 5 6 7 8 9 10 -17 k[m 3 s -1 ] PTB7:PC! with additive 71BM ~ T=300 K
  • 24. Trap Tail States by Thermally Stimulated Currents Trapping is Important Trap density = Lower Limit Shape roughly exponential, energy tail ~90 meV 16Julia Rauh 10 21 2 3 4 5 6 7 8 9 10 22 trapdensity[m -3 ] 0.300.250.200.150.100.050.00 Energy [eV] PTB7:PC70BM with DIO
  • 25. Transient Absorption Nongeminate Decay Dynamics 17 4 6 8 10 -5 2 4 6 8 10 -4 2 4 6 8 ΔOD[a.U] 10 -7 10 -6 10 -5 10 -4 10 -3 Time [s] PTB7:PC71BM with additive 300K 150K 4.5K Clemens Grünewald, Julia Kern
  • 26. Transient Absorption Nongeminate Decay Dynamics 17 4 6 8 10 -5 2 4 6 8 10 -4 2 4 6 8 ΔOD[a.U] 10 -7 10 -6 10 -5 10 -4 10 -3 Time [s] PTB7:PC71BM with additive 300K 150K 4.5K fast free–free (Langevin type) recombination Clemens Grünewald, Julia Kern
  • 27. Transient Absorption Nongeminate Decay Dynamics 17 4 6 8 10 -5 2 4 6 8 10 -4 2 4 6 8 ΔOD[a.U] 10 -7 10 -6 10 -5 10 -4 10 -3 Time [s] PTB7:PC71BM with additive 300K 150K 4.5K fast free–free (Langevin type) recombination slow free–trapped recombination Clemens Grünewald, Julia Kern
  • 28. Outline 18 conclusions implications on organic solar cell performance nongeminate recombination with additive geminate recombination without additive
  • 29. PTB7:PC70BM 1:1.5 w/o additive I–V Reconstruction Why? 19 reconstruction incomplete j(V ) = jsc jloss (n(V )) -50 -40 -30 -20 -10 0 10 CurrentDensity[A/m 2 ] 0.80.60.40.2 Voltage [V] meas. PL reconstr. 0.56 sun 0.32 sun 0.18 sun 0.03 sun
  • 30. PTB7:PC70BM 1:1.5 w/o additive I–V Reconstruction Why? 19 reconstruction incomplete j(V ) = jsc jloss (n(V )) -50 -40 -30 -20 -10 0 10 CurrentDensity[A/m 2 ] 0.80.60.40.2 Voltage [V] meas. PL reconstr. 0.56 sun 0.32 sun 0.18 sun 0.03 sun 1.0 0.8 0.6 0.4 0.2 measured/reconstructed 0.80.60.40.2 Voltage [V] ratio PL Voc 0.03 sun 0.18 sun 0.32 sun 0.56 sun 1 sun First try:
  • 31. Time Delayed Collection Field → P(V) Main Reason: Photogeneration w/out additive: voltage dependent photogeneration 20Alex Förtig 5 6 7 8 9 1 Qtot/Q(-5V) -5 -4 -3 -2 -1 0 prebias voltage [V] w/o add data fit with add data origin unclear
  • 32. j(V ) = e Z (G R) dx ⇡ jgen jloss(V ) jgen ⇡ jsc Current–Voltage Reconstruction ... 21 From the continuity equation: Voltage Current jloss(V ) / n(V ) ⌧(n)
  • 33. j(V ) = e Z (G R) dx ⇡ jgen(V ) jloss(V ) Current–Voltage Reconstruction ... 22 From the continuity equation: jloss(V ) / n(V ) ⌧(n) Voltage Current jgen(V ) ⇡ jsc · P(V )
  • 34. Time Delayed Collection Field Reconstruction incl. Geminate Loss 23 5 6 7 8 9 1 Qtot/Q(-5V) -5 -4 -3 -2 -1 0 prebias voltage [V] w/o add data fit with add data
  • 35. Time Delayed Collection Field Reconstruction incl. Geminate Loss 23 5 6 7 8 9 1 Qtot/Q(-5V) -5 -4 -3 -2 -1 0 prebias voltage [V] w/o add data fit with add data -80 -60 -40 -20 0 currentdensity[A/m 2 ] 0.80.60.40.2 voltage [V] 0.18 sun 1 sun w/o Add measurement reconstruction j (V)gen
  • 36. 2 4 10 21 2 4 10 22 0.80.60.40.20.0 voltage [V] 10 21 2 4 10 22 2 4 chargecarrierdensity[m -3 ] with add w/o add 0.03 sun 1 sun What if... reverse reconstruction: n(V) from I(V) 24Alex Förtig incomplete extraction
  • 37. „Nanomorphology“ by PL 25Björn Gieseking 1.0 0.8 0.6 0.4 0.2 0.0 Photoluminescence(norm.) 2.01.81.61.41.2 Energy / eV 1.0 0.5 0.0 1100 1000 900 800 750 700 650 Wavelength / nm w/o add.3 % DIO PTB7 PC71BM
  • 38. „Nanomorphology“ by PL additive: relative decrease of fullerene PL → smaller fullerene domains 25Björn Gieseking 1.0 0.8 0.6 0.4 0.2 0.0 Photoluminescence(norm.) 2.01.81.61.41.2 Energy / eV 1.0 0.5 0.0 1100 1000 900 800 750 700 650 Wavelength / nm w/o add.3 % DIO PTB7 PC71BM
  • 39. ...on fullerene islands Scenario: Spatial Trapping... without additive 26 Fullerene Polymer Aluminium Cathode Transparent Anode Fullerene Polymer Aluminium Cathode Transparent Anode with additive
  • 40. Conclusions 27 with additive, 7.1% w/o additive, 3.8%            
  • 41. Conclusions 27 with additive, 7.1% w/o additive, 3.8%             nongeminate recombination free carrier and trap assisted recombination
  • 42. Conclusions 27 with additive, 7.1% w/o additive, 3.8%             nongeminate recombination free carrier and trap assisted recombination geminate & nongeminate field dependent photogeneration spatial trapping on fullerene
  • 43. Thanks to Prof. Dyakonov and Würzburg group! Thank you! deibel@disorderedmatter.eu Bayerische Akademie der Wissenschaften EU, DBU, Elite network Bavaria