Chosen Fixed Point
Here is the data for the chosen fixed point.
$F_{UV}$ represents the flavor symmetries in the UV Lagrangian, and $F_{IR}$ represents the flavor symmetries in the IR. $F_{UV}$ and $F_{IR}$ can differ due to accidental symmetry enhancement.
The number of marginal operators, $n_{marginal}$, minus the dimension of flavor symmetries in IR, $|F_{IR}|$, corresponds to the coefficient of $t^6$ in the superconformal index.
| # | Theory | Superpotential | Central charge $a$ | Central charge $c$ | Ratio $a/c$ | Matter field: $R$-charge | U(1) part of $F_{UV}$ | Rank of $F_{UV}$ | Rational |
|---|---|---|---|---|---|---|---|---|---|
| 1504 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{5}\phi_{1}^{2}$ + ${ }M_{1}^{2}$ + ${ }M_{2}M_{4}$ + ${ }M_{4}M_{6}$ | 0.7022 | 0.8628 | 0.8139 | [M:[1.0, 0.9445, 0.889, 1.0555, 1.0277, 0.9445], q:[0.5694, 0.4306], qb:[0.5416, 0.5139], phi:[0.4861]] | [M:[[0], [-4], [-8], [4], [2], [-4]], q:[[5], [-5]], qb:[[3], [1]], phi:[[-1]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{3}$, ${ }M_{2}$, ${ }M_{6}$, ${ }\phi_{1}^{2}$, ${ }M_{1}$, ${ }M_{5}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}^{2}$, ${ }M_{3}^{2}$, ${ }M_{2}M_{3}$, ${ }M_{3}M_{6}$, ${ }M_{2}^{2}$, ${ }M_{1}M_{3}$, ${ }M_{2}M_{6}$, ${ }M_{6}^{2}$, ${ }M_{3}M_{5}$, ${ }M_{2}\phi_{1}^{2}$, ${ }M_{6}\phi_{1}^{2}$, ${ }M_{1}M_{2}$, ${ }M_{1}M_{6}$, ${ }\phi_{1}^{4}$, ${ }M_{2}M_{5}$, ${ }M_{5}M_{6}$, ${ }M_{1}\phi_{1}^{2}$, ${ }M_{3}q_{1}\tilde{q}_{2}$ | ${}$ | -2 | t^2.667 + 2*t^2.834 + t^2.917 + t^3. + t^3.083 + t^3.25 + t^4.042 + t^4.292 + t^4.375 + t^4.458 + t^4.542 + t^4.625 + 2*t^4.708 + t^4.791 + t^4.875 + t^5.334 + 2*t^5.501 + 3*t^5.667 + 2*t^5.75 + 2*t^5.834 + 2*t^5.917 - 2*t^6. + t^6.083 - t^6.416 + t^6.499 + t^6.709 + 2*t^6.876 + 2*t^6.959 + t^7.042 + 2*t^7.125 + 2*t^7.209 + 4*t^7.292 + 3*t^7.375 + t^7.458 + 4*t^7.542 + 2*t^7.625 + 3*t^7.708 + t^7.791 + t^7.958 + t^8.001 + t^8.084 + t^8.124 + 2*t^8.168 + 4*t^8.334 + t^8.417 + 4*t^8.501 + 3*t^8.584 + 5*t^8.75 - 4*t^8.834 - t^4.458/y - t^7.125/y - t^7.292/y + t^7.625/y + t^7.791/y + (2*t^8.501)/y + t^8.584/y + (2*t^8.667)/y + (3*t^8.75)/y + (2*t^8.834)/y + (4*t^8.917)/y - t^4.458*y - t^7.125*y - t^7.292*y + t^7.625*y + t^7.791*y + 2*t^8.501*y + t^8.584*y + 2*t^8.667*y + 3*t^8.75*y + 2*t^8.834*y + 4*t^8.917*y | t^2.667/g1^8 + (2*t^2.834)/g1^4 + t^2.917/g1^2 + t^3. + g1^2*t^3.083 + g1^6*t^3.25 + t^4.042/g1^11 + t^4.292/g1^5 + t^4.375/g1^3 + t^4.458/g1 + g1*t^4.542 + g1^3*t^4.625 + 2*g1^5*t^4.708 + g1^7*t^4.791 + g1^9*t^4.875 + t^5.334/g1^16 + (2*t^5.501)/g1^12 + (3*t^5.667)/g1^8 + (2*t^5.75)/g1^6 + (2*t^5.834)/g1^4 + (2*t^5.917)/g1^2 - 2*t^6. + g1^2*t^6.083 - g1^10*t^6.416 + g1^12*t^6.499 + t^6.709/g1^19 + (2*t^6.876)/g1^15 + (2*t^6.959)/g1^13 + t^7.042/g1^11 + (2*t^7.125)/g1^9 + (2*t^7.209)/g1^7 + (4*t^7.292)/g1^5 + (3*t^7.375)/g1^3 + t^7.458/g1 + 4*g1*t^7.542 + 2*g1^3*t^7.625 + 3*g1^5*t^7.708 + g1^7*t^7.791 + g1^11*t^7.958 + t^8.001/g1^24 + t^8.084/g1^22 + g1^15*t^8.124 + (2*t^8.168)/g1^20 + (4*t^8.334)/g1^16 + t^8.417/g1^14 + (4*t^8.501)/g1^12 + (3*t^8.584)/g1^10 + (5*t^8.75)/g1^6 - (4*t^8.834)/g1^4 - t^4.458/(g1*y) - t^7.125/(g1^9*y) - t^7.292/(g1^5*y) + (g1^3*t^7.625)/y + (g1^7*t^7.791)/y + (2*t^8.501)/(g1^12*y) + t^8.584/(g1^10*y) + (2*t^8.667)/(g1^8*y) + (3*t^8.75)/(g1^6*y) + (2*t^8.834)/(g1^4*y) + (4*t^8.917)/(g1^2*y) - (t^4.458*y)/g1 - (t^7.125*y)/g1^9 - (t^7.292*y)/g1^5 + g1^3*t^7.625*y + g1^7*t^7.791*y + (2*t^8.501*y)/g1^12 + (t^8.584*y)/g1^10 + (2*t^8.667*y)/g1^8 + (3*t^8.75*y)/g1^6 + (2*t^8.834*y)/g1^4 + (4*t^8.917*y)/g1^2 |
Deformation
Here is the data for the deformed fixed points from the chosen fixed point.
| # | Superpotential | Central Charge $a$ | Central Charge $c$ | Ratio $a/c$ | $R$-charges | Superconformal Index | More Info. | Rational |
|---|
Equivalent Fixed Points from Other Seed Theories
Here is a list of equivalent fixed points from other gauge theories.
| # | Theory | Superpotential | Central Charge $a$ | Central Charge $c$ | Ratio $a/c$ | $R$-charges | Superconformal Index | More Info. | Rational |
|---|
Equivalent Fixed Points from the Same Seed Theory
Below is a list of equivalent fixed points from the same seed theories.
| id | Theory | Superpotential | Central Charge $a$ | Central Charge $c$ | Ratio $a/c$ | $R$-charges | More Info. | Rational |
|---|
Previous Theory
The previous fixed point before deforming to get the chosen fixed point.
| # | Theory | Superpotential | Central Charge $a$ | Central Charge $c$ | Ratio $a/c$ | $R$-charges | Superconformal Index | More Info. | Rational |
|---|---|---|---|---|---|---|---|---|---|
| 968 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{5}\phi_{1}^{2}$ + ${ }M_{1}^{2}$ + ${ }M_{2}M_{4}$ | 0.6976 | 0.8545 | 0.8164 | [M:[1.0, 0.9574, 0.9148, 1.0426, 1.0213], q:[0.5533, 0.4467], qb:[0.532, 0.5107], phi:[0.4893]] | t^2.744 + t^2.872 + t^2.936 + t^3. + t^3.064 + t^3.128 + t^3.192 + t^4.149 + t^4.34 + t^4.404 + t^4.468 + t^4.532 + t^4.596 + 2*t^4.66 + t^4.724 + t^4.788 + t^5.489 + t^5.617 + t^5.744 + t^5.808 + 2*t^5.872 + t^5.936 - t^6. - t^4.468/y - t^4.468*y | detail |