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 |
|---|---|---|---|---|---|---|---|---|---|
| 58954 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{5}\phi_{1}q_{1}q_{2}$ + ${ }M_{6}\phi_{1}^{2}$ + ${ }M_{7}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{4}M_{8}$ | 0.6751 | 0.8497 | 0.7945 | [M:[1.1643, 1.0685, 0.8357, 0.7944, 0.6986, 1.0685, 0.6986, 1.2056], q:[0.3972, 0.4384], qb:[0.5343, 0.7671], phi:[0.4657]] | [M:[[-5], [4], [5], [-12], [-3], [4], [-3], [12]], q:[[-6], [11]], qb:[[2], [1]], phi:[[-2]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{5}$, ${ }M_{7}$, ${ }M_{3}$, ${ }q_{2}\tilde{q}_{1}$, ${ }M_{2}$, ${ }M_{6}$, ${ }M_{1}$, ${ }M_{8}$, ${ }\phi_{1}q_{1}^{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }M_{5}^{2}$, ${ }M_{5}M_{7}$, ${ }M_{7}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{3}M_{5}$, ${ }M_{3}M_{7}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{3}^{2}$, ${ }M_{5}q_{2}\tilde{q}_{1}$, ${ }M_{7}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{2}M_{5}$, ${ }M_{5}M_{6}$, ${ }M_{2}M_{7}$, ${ }M_{6}M_{7}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{3}q_{2}\tilde{q}_{1}$, ${ }M_{1}M_{5}$, ${ }M_{1}M_{7}$, ${ }M_{2}M_{3}$, ${ }M_{3}M_{6}$, ${ }M_{5}M_{8}$, ${ }M_{7}M_{8}$, ${ }q_{2}^{2}\tilde{q}_{1}^{2}$, ${ }M_{5}\phi_{1}q_{1}^{2}$, ${ }M_{7}\phi_{1}q_{1}^{2}$ | ${}$ | -2 | 2*t^2.096 + t^2.507 + t^2.918 + 2*t^3.206 + t^3.493 + t^3.617 + t^3.78 + t^4.028 + 4*t^4.192 + t^4.315 + 3*t^4.603 + 3*t^5.014 + 4*t^5.301 + t^5.425 + t^5.589 + 3*t^5.713 + t^5.836 + t^5.876 - 2*t^6. + 4*t^6.124 + 5*t^6.287 + 3*t^6.411 + 2*t^6.535 + 6*t^6.699 + 2*t^6.822 + t^6.946 + 4*t^7.11 + 3*t^7.233 + 5*t^7.397 + 4*t^7.521 + t^7.561 + t^7.645 + 5*t^7.808 + 3*t^7.932 + 2*t^7.972 + t^8.056 - 6*t^8.096 + 7*t^8.22 + 2*t^8.343 + 6*t^8.383 + t^8.507 + 6*t^8.631 + t^8.754 + 7*t^8.794 + t^8.918 - t^4.397/y - (2*t^6.493)/y + (2*t^7.192)/y + t^7.603/y + (2*t^8.014)/y + (6*t^8.301)/y + t^8.425/y - t^8.589/y + (4*t^8.713)/y + (2*t^8.876)/y - t^4.397*y - 2*t^6.493*y + 2*t^7.192*y + t^7.603*y + 2*t^8.014*y + 6*t^8.301*y + t^8.425*y - t^8.589*y + 4*t^8.713*y + 2*t^8.876*y | (2*t^2.096)/g1^3 + g1^5*t^2.507 + g1^13*t^2.918 + 2*g1^4*t^3.206 + t^3.493/g1^5 + g1^12*t^3.617 + t^3.78/g1^14 + g1^20*t^4.028 + (4*t^4.192)/g1^6 + g1^11*t^4.315 + 3*g1^2*t^4.603 + 3*g1^10*t^5.014 + 4*g1*t^5.301 + g1^18*t^5.425 + t^5.589/g1^8 + 3*g1^9*t^5.713 + g1^26*t^5.836 + t^5.876/g1^17 - 2*t^6. + 4*g1^17*t^6.124 + (5*t^6.287)/g1^9 + 3*g1^8*t^6.411 + 2*g1^25*t^6.535 + (6*t^6.699)/g1 + 2*g1^16*t^6.822 + g1^33*t^6.946 + 4*g1^7*t^7.11 + 3*g1^24*t^7.233 + (5*t^7.397)/g1^2 + 4*g1^15*t^7.521 + t^7.561/g1^28 + g1^32*t^7.645 + 5*g1^6*t^7.808 + 3*g1^23*t^7.932 + (2*t^7.972)/g1^20 + g1^40*t^8.056 - (6*t^8.096)/g1^3 + 7*g1^14*t^8.22 + 2*g1^31*t^8.343 + (6*t^8.383)/g1^12 + g1^5*t^8.507 + 6*g1^22*t^8.631 + g1^39*t^8.754 + (7*t^8.794)/g1^4 + g1^13*t^8.918 - t^4.397/(g1^2*y) - (2*t^6.493)/(g1^5*y) + (2*t^7.192)/(g1^6*y) + (g1^2*t^7.603)/y + (2*g1^10*t^8.014)/y + (6*g1*t^8.301)/y + (g1^18*t^8.425)/y - t^8.589/(g1^8*y) + (4*g1^9*t^8.713)/y + (2*t^8.876)/(g1^17*y) - (t^4.397*y)/g1^2 - (2*t^6.493*y)/g1^5 + (2*t^7.192*y)/g1^6 + g1^2*t^7.603*y + 2*g1^10*t^8.014*y + 6*g1*t^8.301*y + g1^18*t^8.425*y - (t^8.589*y)/g1^8 + 4*g1^9*t^8.713*y + (2*t^8.876*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 |
|---|---|---|---|---|---|---|---|---|---|
| 57069 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{5}\phi_{1}q_{1}q_{2}$ + ${ }M_{6}\phi_{1}^{2}$ + ${ }M_{7}\tilde{q}_{1}\tilde{q}_{2}$ | 0.6926 | 0.8801 | 0.7869 | [M:[1.155, 1.076, 0.845, 0.7721, 0.693, 1.076, 0.693], q:[0.3861, 0.4589], qb:[0.538, 0.769], phi:[0.462]] | 2*t^2.079 + t^2.316 + t^2.535 + t^2.991 + 2*t^3.228 + t^3.465 + t^3.702 + t^4.139 + 4*t^4.158 + t^4.377 + 2*t^4.395 + 3*t^4.614 + t^4.633 + t^4.851 + 3*t^5.07 + 5*t^5.307 + t^5.525 + 3*t^5.544 + t^5.763 + 2*t^5.781 + t^5.981 - 2*t^6. - t^4.386/y - t^4.386*y | detail |