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 |
|---|---|---|---|---|---|---|---|---|---|
| 6412 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{5}$ + ${ }\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{6}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}M_{5}$ + ${ }M_{7}\phi_{1}\tilde{q}_{1}^{2}$ + ${ }M_{8}\phi_{1}^{2}$ + ${ }M_{9}\phi_{1}q_{2}^{2}$ | 0.7096 | 0.9074 | 0.7819 | [M:[0.9825, 0.8166, 0.9825, 0.8166, 1.1834, 0.7336, 0.7336, 1.1004, 0.7336], q:[0.6092, 0.4083], qb:[0.4083, 0.7751], phi:[0.4498]] | [M:[[-22], [-2], [-22], [-2], [2], [8], [8], [12], [8]], q:[[23], [-1]], qb:[[-1], [3]], phi:[[-6]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{6}$, ${ }M_{7}$, ${ }M_{9}$, ${ }M_{2}$, ${ }M_{4}$, ${ }M_{1}$, ${ }M_{3}$, ${ }M_{8}$, ${ }M_{5}$, ${ }q_{1}\tilde{q}_{2}$, ${ }M_{6}^{2}$, ${ }M_{6}M_{7}$, ${ }M_{7}^{2}$, ${ }M_{6}M_{9}$, ${ }M_{7}M_{9}$, ${ }M_{9}^{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }M_{2}M_{6}$, ${ }M_{4}M_{6}$, ${ }M_{2}M_{7}$, ${ }M_{4}M_{7}$, ${ }M_{2}M_{9}$, ${ }M_{4}M_{9}$, ${ }M_{2}^{2}$, ${ }M_{2}M_{4}$, ${ }M_{4}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}^{2}$, ${ }M_{1}M_{6}$, ${ }M_{3}M_{6}$, ${ }M_{1}M_{7}$, ${ }M_{3}M_{7}$, ${ }M_{1}M_{9}$, ${ }M_{3}M_{9}$, ${ }M_{1}M_{2}$, ${ }M_{2}M_{3}$, ${ }M_{1}M_{4}$, ${ }M_{3}M_{4}$, ${ }M_{6}M_{8}$, ${ }M_{7}M_{8}$, ${ }M_{8}M_{9}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }M_{5}M_{6}$, ${ }M_{5}M_{7}$, ${ }M_{2}M_{8}$, ${ }M_{4}M_{8}$, ${ }M_{5}M_{9}$, ${ }M_{1}^{2}$, ${ }M_{1}M_{3}$, ${ }M_{3}^{2}$ | ${}$ | -3 | 3*t^2.201 + 2*t^2.45 + 2*t^2.948 + t^3.301 + t^3.55 + t^4.153 + 8*t^4.402 + 6*t^4.651 + 3*t^4.9 + t^5.004 + 6*t^5.148 + 2*t^5.397 + 3*t^5.502 + 5*t^5.751 + 3*t^5.895 - 3*t^6. + 3*t^6.354 + t^6.498 + 16*t^6.603 - 2*t^6.747 + 14*t^6.852 + 7*t^7.1 + 3*t^7.205 + 14*t^7.349 + 2*t^7.454 + 5*t^7.598 + 7*t^7.703 + 2*t^7.847 + 10*t^7.952 + 9*t^8.096 - 10*t^8.201 + t^8.306 + 3*t^8.345 - 7*t^8.45 + 7*t^8.555 + t^8.699 + 26*t^8.804 + 4*t^8.843 - 13*t^8.948 - t^4.349/y - (3*t^6.55)/y - t^6.799/y - (2*t^7.297)/y + (5*t^7.402)/y + (6*t^7.651)/y + (2*t^7.9)/y + (9*t^8.148)/y + (4*t^8.397)/y + (3*t^8.502)/y - t^8.751/y + t^8.895/y - t^4.349*y - 3*t^6.55*y - t^6.799*y - 2*t^7.297*y + 5*t^7.402*y + 6*t^7.651*y + 2*t^7.9*y + 9*t^8.148*y + 4*t^8.397*y + 3*t^8.502*y - t^8.751*y + t^8.895*y | 3*g1^8*t^2.201 + (2*t^2.45)/g1^2 + (2*t^2.948)/g1^22 + g1^12*t^3.301 + g1^2*t^3.55 + g1^26*t^4.153 + 8*g1^16*t^4.402 + 6*g1^6*t^4.651 + (3*t^4.9)/g1^4 + g1^40*t^5.004 + (6*t^5.148)/g1^14 + (2*t^5.397)/g1^24 + 3*g1^20*t^5.502 + 5*g1^10*t^5.751 + (3*t^5.895)/g1^44 - 3*t^6. + 3*g1^34*t^6.354 + t^6.498/g1^20 + 16*g1^24*t^6.603 - (2*t^6.747)/g1^30 + 14*g1^14*t^6.852 + 7*g1^4*t^7.1 + 3*g1^48*t^7.205 + (14*t^7.349)/g1^6 + 2*g1^38*t^7.454 + (5*t^7.598)/g1^16 + 7*g1^28*t^7.703 + (2*t^7.847)/g1^26 + 10*g1^18*t^7.952 + (9*t^8.096)/g1^36 - 10*g1^8*t^8.201 + g1^52*t^8.306 + (3*t^8.345)/g1^46 - (7*t^8.45)/g1^2 + 7*g1^42*t^8.555 + t^8.699/g1^12 + 26*g1^32*t^8.804 + (4*t^8.843)/g1^66 - (13*t^8.948)/g1^22 - t^4.349/(g1^6*y) - (3*g1^2*t^6.55)/y - t^6.799/(g1^8*y) - (2*t^7.297)/(g1^28*y) + (5*g1^16*t^7.402)/y + (6*g1^6*t^7.651)/y + (2*t^7.9)/(g1^4*y) + (9*t^8.148)/(g1^14*y) + (4*t^8.397)/(g1^24*y) + (3*g1^20*t^8.502)/y - (g1^10*t^8.751)/y + t^8.895/(g1^44*y) - (t^4.349*y)/g1^6 - 3*g1^2*t^6.55*y - (t^6.799*y)/g1^8 - (2*t^7.297*y)/g1^28 + 5*g1^16*t^7.402*y + 6*g1^6*t^7.651*y + (2*t^7.9*y)/g1^4 + (9*t^8.148*y)/g1^14 + (4*t^8.397*y)/g1^24 + 3*g1^20*t^8.502*y - g1^10*t^8.751*y + (t^8.895*y)/g1^44 |
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 |
|---|---|---|---|---|---|---|---|---|---|
| 4771 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{5}$ + ${ }\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{6}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}M_{5}$ + ${ }M_{7}\phi_{1}\tilde{q}_{1}^{2}$ + ${ }M_{8}\phi_{1}^{2}$ | 0.69 | 0.8709 | 0.7922 | [M:[0.9757, 0.816, 0.9757, 0.816, 1.184, 0.7361, 0.7361, 1.1042], q:[0.6164, 0.408], qb:[0.408, 0.776], phi:[0.4479]] | 2*t^2.208 + 2*t^2.448 + 2*t^2.927 + t^3.313 + t^3.552 + t^3.792 + t^4.177 + 5*t^4.417 + 4*t^4.656 + 3*t^4.896 + t^5.042 + 4*t^5.135 + 2*t^5.375 + 2*t^5.521 + 4*t^5.76 + 3*t^5.854 - t^6. - t^4.344/y - t^4.344*y | detail |