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 |
|---|---|---|---|---|---|---|---|---|---|
| 55665 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{5}\phi_{1}^{2}$ + ${ }M_{6}\phi_{1}q_{1}^{2}$ | 0.6703 | 0.8361 | 0.8016 | [M:[1.1634, 1.0692, 0.8366, 0.7923, 1.0692, 0.7424], q:[0.3961, 0.4404], qb:[0.5346, 0.7673], phi:[0.4654]] | [M:[[-5], [4], [5], [-12], [4], [14]], q:[[-6], [11]], qb:[[2], [1]], phi:[[-2]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{6}$, ${ }M_{4}$, ${ }M_{3}$, ${ }q_{2}\tilde{q}_{1}$, ${ }M_{2}$, ${ }M_{5}$, ${ }M_{1}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{6}^{2}$, ${ }M_{4}M_{6}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{3}M_{6}$, ${ }M_{4}^{2}$, ${ }M_{3}M_{4}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }M_{3}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{6}q_{2}\tilde{q}_{1}$, ${ }M_{4}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{2}M_{6}$, ${ }M_{5}M_{6}$, ${ }M_{3}q_{2}\tilde{q}_{1}$, ${ }M_{2}M_{4}$, ${ }M_{4}M_{5}$, ${ }M_{2}M_{3}$, ${ }M_{3}M_{5}$, ${ }M_{1}M_{6}$, ${ }q_{2}^{2}\tilde{q}_{1}^{2}$ | ${}$ | -2 | t^2.227 + t^2.377 + t^2.51 + t^2.925 + 2*t^3.208 + t^3.49 + 2*t^3.906 + t^4.039 + t^4.188 + t^4.321 + t^4.454 + 2*t^4.604 + t^4.737 + t^4.754 + t^4.886 + t^5.019 + t^5.152 + t^5.302 + 3*t^5.435 + t^5.585 + 2*t^5.717 + t^5.85 - 2*t^6. + 3*t^6.133 + t^6.266 + 5*t^6.415 + 2*t^6.548 + t^6.565 + t^6.681 + t^6.698 + 4*t^6.831 + 2*t^6.964 + 3*t^7.114 + t^7.13 + 3*t^7.246 + t^7.379 + t^7.396 + 3*t^7.529 + 3*t^7.662 + 3*t^7.812 + 4*t^7.944 + t^7.961 + 2*t^8.077 + 5*t^8.36 - 3*t^8.377 + t^8.493 - t^8.51 + 6*t^8.643 + 3*t^8.775 + 2*t^8.792 + t^8.908 + t^8.925 + t^8.942 - t^4.396/y - t^6.623/y - t^6.773/y + t^7.188/y + t^7.737/y + t^7.886/y + t^8.019/y + t^8.152/y + t^8.169/y + t^8.302/y + (3*t^8.435)/y + (2*t^8.585)/y + (3*t^8.717)/y - t^8.85/y + t^8.867/y - t^4.396*y - t^6.623*y - t^6.773*y + t^7.188*y + t^7.737*y + t^7.886*y + t^8.019*y + t^8.152*y + t^8.169*y + t^8.302*y + 3*t^8.435*y + 2*t^8.585*y + 3*t^8.717*y - t^8.85*y + t^8.867*y | g1^14*t^2.227 + t^2.377/g1^12 + g1^5*t^2.51 + g1^13*t^2.925 + 2*g1^4*t^3.208 + t^3.49/g1^5 + 2*g1^3*t^3.906 + g1^20*t^4.039 + t^4.188/g1^6 + g1^11*t^4.321 + g1^28*t^4.454 + 2*g1^2*t^4.604 + g1^19*t^4.737 + t^4.754/g1^24 + t^4.886/g1^7 + g1^10*t^5.019 + g1^27*t^5.152 + g1*t^5.302 + 3*g1^18*t^5.435 + t^5.585/g1^8 + 2*g1^9*t^5.717 + g1^26*t^5.85 - 2*t^6. + 3*g1^17*t^6.133 + g1^34*t^6.266 + 5*g1^8*t^6.415 + 2*g1^25*t^6.548 + t^6.565/g1^18 + g1^42*t^6.681 + t^6.698/g1 + 4*g1^16*t^6.831 + 2*g1^33*t^6.964 + 3*g1^7*t^7.114 + t^7.13/g1^36 + 3*g1^24*t^7.246 + g1^41*t^7.379 + t^7.396/g1^2 + 3*g1^15*t^7.529 + 3*g1^32*t^7.662 + 3*g1^6*t^7.812 + 4*g1^23*t^7.944 + t^7.961/g1^20 + 2*g1^40*t^8.077 + 5*g1^31*t^8.36 - (3*t^8.377)/g1^12 + g1^48*t^8.493 - g1^5*t^8.51 + 6*g1^22*t^8.643 + 3*g1^39*t^8.775 + (2*t^8.792)/g1^4 + g1^56*t^8.908 + g1^13*t^8.925 + t^8.942/g1^30 - t^4.396/(g1^2*y) - (g1^12*t^6.623)/y - t^6.773/(g1^14*y) + t^7.188/(g1^6*y) + (g1^19*t^7.737)/y + t^7.886/(g1^7*y) + (g1^10*t^8.019)/y + (g1^27*t^8.152)/y + t^8.169/(g1^16*y) + (g1*t^8.302)/y + (3*g1^18*t^8.435)/y + (2*t^8.585)/(g1^8*y) + (3*g1^9*t^8.717)/y - (g1^26*t^8.85)/y + t^8.867/(g1^17*y) - (t^4.396*y)/g1^2 - g1^12*t^6.623*y - (t^6.773*y)/g1^14 + (t^7.188*y)/g1^6 + g1^19*t^7.737*y + (t^7.886*y)/g1^7 + g1^10*t^8.019*y + g1^27*t^8.152*y + (t^8.169*y)/g1^16 + g1*t^8.302*y + 3*g1^18*t^8.435*y + (2*t^8.585*y)/g1^8 + 3*g1^9*t^8.717*y - g1^26*t^8.85*y + (t^8.867*y)/g1^17 |
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 |
|---|---|---|---|---|---|---|---|---|---|
| 48133 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{5}\phi_{1}^{2}$ | 0.6513 | 0.8005 | 0.8136 | [M:[1.1562, 1.075, 0.8438, 0.7749, 1.075], q:[0.3875, 0.4563], qb:[0.5375, 0.7688], phi:[0.4625]] | t^2.325 + t^2.531 + t^2.981 + 2*t^3.225 + t^3.469 + t^3.712 + 2*t^3.919 + t^4.125 + t^4.162 + t^4.369 + t^4.613 + t^4.65 + t^4.856 + t^5.063 + t^5.306 + t^5.513 + t^5.55 + t^5.756 + t^5.963 - 2*t^6. - t^4.387/y - t^4.387*y | detail |