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 |
|---|---|---|---|---|---|---|---|---|---|
| 46161 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }\phi_{1}q_{1}^{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{1}\phi_{1}^{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }q_{1}q_{2}\tilde{q}_{2}^{2}$ | 0.6055 | 0.7763 | 0.78 | [M:[0.9922, 1.0233, 0.7714], q:[0.7481, 0.2597], qb:[0.4806, 0.4961], phi:[0.5039]] | [M:[[4], [-12], [-11]], q:[[1], [-5]], qb:[[10], [2]], phi:[[-2]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}q_{2}\tilde{q}_{1}$, ${ }q_{2}\tilde{q}_{2}$, ${ }M_{3}$, ${ }M_{1}$, ${ }\phi_{1}^{2}$, ${ }M_{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }q_{2}^{2}\tilde{q}_{1}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }M_{3}q_{2}\tilde{q}_{1}$, ${ }q_{2}^{2}\tilde{q}_{2}^{2}$, ${ }M_{3}q_{2}\tilde{q}_{2}$, ${ }M_{3}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }M_{1}M_{3}$, ${ }\phi_{1}q_{2}^{3}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }M_{3}\phi_{1}^{2}$, ${ }\phi_{1}q_{2}^{3}\tilde{q}_{2}$, ${ }M_{2}M_{3}$, ${ }M_{3}\phi_{1}q_{2}^{2}$, ${ }M_{1}^{2}$, ${ }\phi_{1}q_{2}^{2}\tilde{q}_{1}^{2}$ | ${}\phi_{1}q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$ | 0 | t^2.221 + t^2.267 + t^2.314 + t^2.977 + t^3.023 + 2*t^3.07 + 2*t^3.733 + t^3.779 + t^4.395 + 2*t^4.442 + 2*t^4.488 + 2*t^4.535 + t^4.582 + t^4.628 + t^5.198 + 2*t^5.244 + 3*t^5.291 + 2*t^5.337 + 2*t^5.384 + t^5.953 + 3*t^6.047 + 3*t^6.093 + 3*t^6.14 + t^6.616 + t^6.663 + 2*t^6.709 + 3*t^6.756 + 5*t^6.802 + 3*t^6.849 + t^6.896 + t^6.942 + t^7.418 + 3*t^7.465 + 4*t^7.512 + 4*t^7.558 + 4*t^7.605 + 2*t^7.651 + 2*t^7.698 + t^8.128 - t^8.221 + t^8.267 + t^8.314 + 5*t^8.361 + 4*t^8.407 + 3*t^8.454 + t^8.79 + 2*t^8.837 + 2*t^8.883 + t^8.93 - t^8.977 - t^4.512/y - t^6.826/y + t^7.442/y + t^7.488/y + t^7.535/y + (2*t^8.198)/y + (2*t^8.244)/y + (4*t^8.291)/y + (3*t^8.337)/y + (2*t^8.384)/y + (2*t^8.953)/y - t^4.512*y - t^6.826*y + t^7.442*y + t^7.488*y + t^7.535*y + 2*t^8.198*y + 2*t^8.244*y + 4*t^8.291*y + 3*t^8.337*y + 2*t^8.384*y + 2*t^8.953*y | g1^5*t^2.221 + t^2.267/g1^3 + t^2.314/g1^11 + g1^4*t^2.977 + t^3.023/g1^4 + (2*t^3.07)/g1^12 + 2*g1^3*t^3.733 + t^3.779/g1^5 + g1^18*t^4.395 + 2*g1^10*t^4.442 + 2*g1^2*t^4.488 + (2*t^4.535)/g1^6 + t^4.582/g1^14 + t^4.628/g1^22 + g1^9*t^5.198 + 2*g1*t^5.244 + (3*t^5.291)/g1^7 + (2*t^5.337)/g1^15 + (2*t^5.384)/g1^23 + g1^8*t^5.953 + (3*t^6.047)/g1^8 + (3*t^6.093)/g1^16 + (3*t^6.14)/g1^24 + g1^23*t^6.616 + g1^15*t^6.663 + 2*g1^7*t^6.709 + (3*t^6.756)/g1 + (5*t^6.802)/g1^9 + (3*t^6.849)/g1^17 + t^6.896/g1^25 + t^6.942/g1^33 + g1^14*t^7.418 + 3*g1^6*t^7.465 + (4*t^7.512)/g1^2 + (4*t^7.558)/g1^10 + (4*t^7.605)/g1^18 + (2*t^7.651)/g1^26 + (2*t^7.698)/g1^34 + g1^21*t^8.128 - g1^5*t^8.221 + t^8.267/g1^3 + t^8.314/g1^11 + (5*t^8.361)/g1^19 + (4*t^8.407)/g1^27 + (3*t^8.454)/g1^35 + g1^36*t^8.79 + 2*g1^28*t^8.837 + 2*g1^20*t^8.883 + g1^12*t^8.93 - g1^4*t^8.977 - t^4.512/(g1^2*y) - t^6.826/(g1^13*y) + (g1^10*t^7.442)/y + (g1^2*t^7.488)/y + t^7.535/(g1^6*y) + (2*g1^9*t^8.198)/y + (2*g1*t^8.244)/y + (4*t^8.291)/(g1^7*y) + (3*t^8.337)/(g1^15*y) + (2*t^8.384)/(g1^23*y) + (2*g1^8*t^8.953)/y - (t^4.512*y)/g1^2 - (t^6.826*y)/g1^13 + g1^10*t^7.442*y + g1^2*t^7.488*y + (t^7.535*y)/g1^6 + 2*g1^9*t^8.198*y + 2*g1*t^8.244*y + (4*t^8.291*y)/g1^7 + (3*t^8.337*y)/g1^15 + (2*t^8.384*y)/g1^23 + 2*g1^8*t^8.953*y |
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 |
|---|---|---|---|---|---|---|---|---|---|
| 46045 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }\phi_{1}q_{1}^{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{1}\phi_{1}^{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ | 0.6066 | 0.7782 | 0.7795 | [M:[0.9854, 1.0439, 0.7625], q:[0.7463, 0.2683], qb:[0.4911, 0.4649], phi:[0.5073]] | t^2.2 + t^2.278 + t^2.288 + t^2.956 + t^3.044 + 2*t^3.132 + t^3.634 + t^3.722 + t^3.8 + t^4.312 + t^4.39 + t^4.399 + t^4.469 + t^4.478 + t^4.487 + t^4.557 + t^4.566 + t^4.575 + t^5.156 + t^5.234 + 2*t^5.244 + t^5.322 + 2*t^5.332 + t^5.41 + 2*t^5.419 + t^5.834 + t^5.912 + t^5.921 - t^6. - t^4.522/y - t^4.522*y | detail |